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	<title>Astronomy, Vol. 5, Pages 10: Transits of Venus, Solar Diameter and Sky Transparency</title>
	<link>https://www.mdpi.com/2674-0346/5/3/10</link>
	<description>The transits of Venus occur in couples every 105/122 years: the observed ones were in 1639; 1761&amp;amp;ndash;1769; 1874&amp;amp;ndash;1882; and 2004&amp;amp;ndash;2012. The next couple will occur in the years 2117 and 2125. We need all four contacts to determine the solar diameter accurately. The black-drop phenomenon blurs internal contacts, so we developed a parabolic analysis of the chords drawn by the disk of Venus on the solar limb. The extrapolation of the zeroes gives the contact timings. We tested this method with some high-quality images obtained in 2004 and 2012, and we applied it to the observations of 2012 in a visual band (Huairou Solar Observing Station, hazy weather) and H-alpha (Shen Zen Astronomical Observatory). To exclude a reduction in the measured diameter by the haze, we made two series of measures at the Clementine Gnomon (Rome) and at the PHYSIS telescope (Rome), under various sky transparencies and with diffraction-limited instruments. The haze and the low altitudes above the horizon reduced accuracy at all first contacts examined, without changing the solar diameter. Our measures obtained in China during the transit of 2012 yielded a photospheric radius R&amp;amp;#8857;P = 959.33&amp;amp;Prime; &amp;amp;plusmn; 0.06&amp;amp;Prime;, based on 76 + 75 diffraction-limited images; this is compatible with the chromospheric radius measured at the base of the spiculae, which is R&amp;amp;#8857;C = 959.78&amp;amp;Prime; &amp;amp;plusmn; 0.11&amp;amp;Prime;, relying on 7 + 5 diffraction-limited series of images.</description>
	<pubDate>2026-06-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 10: Transits of Venus, Solar Diameter and Sky Transparency</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/3/10">doi: 10.3390/astronomy5030010</a></p>
	<p>Authors:
		Costantino Sigismondi
		Andrea Brucato
		Xiaofan Wang
		Wenbin Xie
		Anthony Ayiomamitis
		Dong Wang
		</p>
	<p>The transits of Venus occur in couples every 105/122 years: the observed ones were in 1639; 1761&amp;amp;ndash;1769; 1874&amp;amp;ndash;1882; and 2004&amp;amp;ndash;2012. The next couple will occur in the years 2117 and 2125. We need all four contacts to determine the solar diameter accurately. The black-drop phenomenon blurs internal contacts, so we developed a parabolic analysis of the chords drawn by the disk of Venus on the solar limb. The extrapolation of the zeroes gives the contact timings. We tested this method with some high-quality images obtained in 2004 and 2012, and we applied it to the observations of 2012 in a visual band (Huairou Solar Observing Station, hazy weather) and H-alpha (Shen Zen Astronomical Observatory). To exclude a reduction in the measured diameter by the haze, we made two series of measures at the Clementine Gnomon (Rome) and at the PHYSIS telescope (Rome), under various sky transparencies and with diffraction-limited instruments. The haze and the low altitudes above the horizon reduced accuracy at all first contacts examined, without changing the solar diameter. Our measures obtained in China during the transit of 2012 yielded a photospheric radius R&amp;amp;#8857;P = 959.33&amp;amp;Prime; &amp;amp;plusmn; 0.06&amp;amp;Prime;, based on 76 + 75 diffraction-limited images; this is compatible with the chromospheric radius measured at the base of the spiculae, which is R&amp;amp;#8857;C = 959.78&amp;amp;Prime; &amp;amp;plusmn; 0.11&amp;amp;Prime;, relying on 7 + 5 diffraction-limited series of images.</p>
	]]></content:encoded>

	<dc:title>Transits of Venus, Solar Diameter and Sky Transparency</dc:title>
			<dc:creator>Costantino Sigismondi</dc:creator>
			<dc:creator>Andrea Brucato</dc:creator>
			<dc:creator>Xiaofan Wang</dc:creator>
			<dc:creator>Wenbin Xie</dc:creator>
			<dc:creator>Anthony Ayiomamitis</dc:creator>
			<dc:creator>Dong Wang</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5030010</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-06-24</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-06-24</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>10</prism:startingPage>
		<prism:doi>10.3390/astronomy5030010</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/3/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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        <item rdf:about="https://www.mdpi.com/2674-0346/5/2/9">

	<title>Astronomy, Vol. 5, Pages 9: Induced-Gravity Palatini-like Higgs Inflation in Supergravity Confronts ACT DR6</title>
	<link>https://www.mdpi.com/2674-0346/5/2/9</link>
	<description>We formulate within Supergravity a model of induced-gravity inflation, excellently consistent with ACT DR6, inspired by the Palatini gravity. The inflaton belongs in the decomposition of a conjugate pair of Higgs superfields which lead to the spontaneous breaking of a U(1)B&amp;amp;minus;L symmetry at a scale close to the range (0.145&amp;amp;ndash;8.35) &amp;amp;times; 1016 GeV. The inflaton field is canonically normalized thanks to one real and shift-symmetric contribution into the K&amp;amp;auml;hler potential. It also includes two separate holomorphic and antiholomorphic logarithmic terms, the argument of which can be interpreted as the coupling of the inflaton to the Ricci scalar. The attainment of inflation allows for subplanckian inflaton values and energy scales below the cut-off scale of the corresponding effective theory. Embedding the model in a B&amp;amp;minus;L extension of the MSSM we show how the &amp;amp;mu; parameter can be generated and non-thermal leptogenesis can be successfully realized. An outcome of our scheme is split SUSY with gravitino mass in the range (40&amp;amp;ndash;60) PeV, which is consistent with the results of LHC on the Higgs boson mass.</description>
	<pubDate>2026-05-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 9: Induced-Gravity Palatini-like Higgs Inflation in Supergravity Confronts ACT DR6</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/2/9">doi: 10.3390/astronomy5020009</a></p>
	<p>Authors:
		Constantinos Pallis
		</p>
	<p>We formulate within Supergravity a model of induced-gravity inflation, excellently consistent with ACT DR6, inspired by the Palatini gravity. The inflaton belongs in the decomposition of a conjugate pair of Higgs superfields which lead to the spontaneous breaking of a U(1)B&amp;amp;minus;L symmetry at a scale close to the range (0.145&amp;amp;ndash;8.35) &amp;amp;times; 1016 GeV. The inflaton field is canonically normalized thanks to one real and shift-symmetric contribution into the K&amp;amp;auml;hler potential. It also includes two separate holomorphic and antiholomorphic logarithmic terms, the argument of which can be interpreted as the coupling of the inflaton to the Ricci scalar. The attainment of inflation allows for subplanckian inflaton values and energy scales below the cut-off scale of the corresponding effective theory. Embedding the model in a B&amp;amp;minus;L extension of the MSSM we show how the &amp;amp;mu; parameter can be generated and non-thermal leptogenesis can be successfully realized. An outcome of our scheme is split SUSY with gravitino mass in the range (40&amp;amp;ndash;60) PeV, which is consistent with the results of LHC on the Higgs boson mass.</p>
	]]></content:encoded>

	<dc:title>Induced-Gravity Palatini-like Higgs Inflation in Supergravity Confronts ACT DR6</dc:title>
			<dc:creator>Constantinos Pallis</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5020009</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-05-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-05-22</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>9</prism:startingPage>
		<prism:doi>10.3390/astronomy5020009</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/2/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/2/8">

	<title>Astronomy, Vol. 5, Pages 8: Cometary Dynamics&amp;mdash;Formation and Evolution of the Oort Cloud</title>
	<link>https://www.mdpi.com/2674-0346/5/2/8</link>
	<description>In this review, the formation of the Oort Cloud is illuminated from several aspects. One is the history of the subject with an outline of the fundamental discoveries by &amp;amp;Ouml;pik, Oort and Hills. It is argued that the basic reason for judging Oort as the real discoverer is that he had access to observational data in the form of original orbits of long period comets. Further landmarks are identified, like the exploration of the role of the Galactic tide in the supply of observable comets by Heisler and Tremaine, the clarification of a synergy between tide and stars as the reason for a continued, efficient supply by Rickman et al., the discovery by Kaib and Quinn that inner core comets become observable due to planetary perturbations, disguised as new comets, and the demonstration of how Oort Cloud formation may work in the realm of the Nice Model by Brasser and Morbidelli. Further discussions refer to the possible role of the Grand Tack model in Oort Cloud formation and recent developments like Pan-STARRS in obtaining better data on very distant comets and Gaia in identifying stellar encounters in the close past and future with ensuing, important modifications of the Oort Cloud. It is finally argued that an important Galactic sculpting has occurred since the primordial Oort Cloud was formed by means of global shake-up events resulting from impulses imparted to the Sun by external perturbers like massive stars or Giant Molecular Clouds, and that this may be the real reason for the survival of an outer halo that reveals the existence of the Oort Cloud through the Oort spike.</description>
	<pubDate>2026-04-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 8: Cometary Dynamics&amp;mdash;Formation and Evolution of the Oort Cloud</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/2/8">doi: 10.3390/astronomy5020008</a></p>
	<p>Authors:
		Hans Rickman
		</p>
	<p>In this review, the formation of the Oort Cloud is illuminated from several aspects. One is the history of the subject with an outline of the fundamental discoveries by &amp;amp;Ouml;pik, Oort and Hills. It is argued that the basic reason for judging Oort as the real discoverer is that he had access to observational data in the form of original orbits of long period comets. Further landmarks are identified, like the exploration of the role of the Galactic tide in the supply of observable comets by Heisler and Tremaine, the clarification of a synergy between tide and stars as the reason for a continued, efficient supply by Rickman et al., the discovery by Kaib and Quinn that inner core comets become observable due to planetary perturbations, disguised as new comets, and the demonstration of how Oort Cloud formation may work in the realm of the Nice Model by Brasser and Morbidelli. Further discussions refer to the possible role of the Grand Tack model in Oort Cloud formation and recent developments like Pan-STARRS in obtaining better data on very distant comets and Gaia in identifying stellar encounters in the close past and future with ensuing, important modifications of the Oort Cloud. It is finally argued that an important Galactic sculpting has occurred since the primordial Oort Cloud was formed by means of global shake-up events resulting from impulses imparted to the Sun by external perturbers like massive stars or Giant Molecular Clouds, and that this may be the real reason for the survival of an outer halo that reveals the existence of the Oort Cloud through the Oort spike.</p>
	]]></content:encoded>

	<dc:title>Cometary Dynamics&amp;amp;mdash;Formation and Evolution of the Oort Cloud</dc:title>
			<dc:creator>Hans Rickman</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5020008</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-04-14</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-04-14</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>8</prism:startingPage>
		<prism:doi>10.3390/astronomy5020008</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/2/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
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	<title>Astronomy, Vol. 5, Pages 7: A Statistical Study of the Jet Structure of Gamma-Ray Bursts</title>
	<link>https://www.mdpi.com/2674-0346/5/2/7</link>
	<description>The jet structure plays an important role in both the prompt and afterglow emission phases of gamma-ray bursts (GRBs). Whether GRB jets are better described by uniform (top-hat) or structured models remains an open question. We use the afterglowpy Python package to numerically model the late X-ray afterglow light curves of a large sample of long and short GRBs, and apply the Bayesian Information Criterion (BIC) to compare the performance of top-hat and Gaussian structured jet models. Within our adopted modeling framework, we find that the top-hat model is preferred by the BIC for &amp;amp;sim;78.9% (150/190) of long GRBs and 70% (7/10) of short GRBs. GRB 180205A and GRB 140515A exhibit &amp;amp;Delta;BIC &amp;amp;lt; 2 for all three model comparisons, indicating that top-hat, Gaussian, and power-law jets provide equivalent fits to their afterglow light curves. This large-sample analysis suggests that uniform jets may be more common than structured jets in the observed GRB population, although this conclusion is subject to the limitations of our model assumptions and the BIC-based model selection criterion. Furthermore, we find that the best-fit distributions of observer angle &amp;amp;theta;obs, electron energy fraction &amp;amp;#1013;e, and isotropic equivalent energy E0 differ significantly between the top-hat and Gaussian jet models, with &amp;amp;theta;obs showing the most pronounced distinction.</description>
	<pubDate>2026-04-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 7: A Statistical Study of the Jet Structure of Gamma-Ray Bursts</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/2/7">doi: 10.3390/astronomy5020007</a></p>
	<p>Authors:
		Mao Liao
		Zhao-Yang Peng
		Jia-Ming Chen
		</p>
	<p>The jet structure plays an important role in both the prompt and afterglow emission phases of gamma-ray bursts (GRBs). Whether GRB jets are better described by uniform (top-hat) or structured models remains an open question. We use the afterglowpy Python package to numerically model the late X-ray afterglow light curves of a large sample of long and short GRBs, and apply the Bayesian Information Criterion (BIC) to compare the performance of top-hat and Gaussian structured jet models. Within our adopted modeling framework, we find that the top-hat model is preferred by the BIC for &amp;amp;sim;78.9% (150/190) of long GRBs and 70% (7/10) of short GRBs. GRB 180205A and GRB 140515A exhibit &amp;amp;Delta;BIC &amp;amp;lt; 2 for all three model comparisons, indicating that top-hat, Gaussian, and power-law jets provide equivalent fits to their afterglow light curves. This large-sample analysis suggests that uniform jets may be more common than structured jets in the observed GRB population, although this conclusion is subject to the limitations of our model assumptions and the BIC-based model selection criterion. Furthermore, we find that the best-fit distributions of observer angle &amp;amp;theta;obs, electron energy fraction &amp;amp;#1013;e, and isotropic equivalent energy E0 differ significantly between the top-hat and Gaussian jet models, with &amp;amp;theta;obs showing the most pronounced distinction.</p>
	]]></content:encoded>

	<dc:title>A Statistical Study of the Jet Structure of Gamma-Ray Bursts</dc:title>
			<dc:creator>Mao Liao</dc:creator>
			<dc:creator>Zhao-Yang Peng</dc:creator>
			<dc:creator>Jia-Ming Chen</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5020007</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-04-03</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-04-03</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>7</prism:startingPage>
		<prism:doi>10.3390/astronomy5020007</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/2/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/6">

	<title>Astronomy, Vol. 5, Pages 6: RadioObservations of Microquasars with FAST</title>
	<link>https://www.mdpi.com/2674-0346/5/1/6</link>
	<description>We report six radio observations of four microquasars&amp;amp;mdash;SS 433, GRS 1915+105, Cyg X-3 and MAXI J1820+070&amp;amp;mdash;conducted between 2022 and 2025 with the Five-hundred-meter Aperture Spherical radio Telescope (FAST) using its pulsar backend, achieving a time resolution of 98.304 &amp;amp;mu;s across an effective feed range of 1.04&amp;amp;ndash;1.45 GHz. A major focus of this work is the development of a standardized calibration pipeline for microquasar observations, including RFI mitigation, flux density, and polarization calibration, as well as multi-beam correlation inspections. Using On&amp;amp;ndash;Off mode and cross-beam verification, radio activity was detected in SS 433, GRS 1915+105 and Cyg X-3, while MAXI J1820+070 remained inactive. Both SS 433 and GRS 1915+105 show low linear polarization degrees of only a few percent. No credible quasi-periodic oscillations (QPOs) were detected in the 0.01&amp;amp;ndash;100 Hz range, suggesting that radio QPOs within this frequency range are relatively rare compared to those observed in the X-ray band. We therefore highlight the importance of future monitoring with high&amp;amp;ndash;time-resolution and high&amp;amp;ndash;sensitivity radio telescopes such as FAST, which will be crucial for revealing the correlation between jet and accretion processes and for uncovering the physical origin of QPOs.</description>
	<pubDate>2026-03-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 6: RadioObservations of Microquasars with FAST</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/6">doi: 10.3390/astronomy5010006</a></p>
	<p>Authors:
		Botao Li
		Wei Wang
		</p>
	<p>We report six radio observations of four microquasars&amp;amp;mdash;SS 433, GRS 1915+105, Cyg X-3 and MAXI J1820+070&amp;amp;mdash;conducted between 2022 and 2025 with the Five-hundred-meter Aperture Spherical radio Telescope (FAST) using its pulsar backend, achieving a time resolution of 98.304 &amp;amp;mu;s across an effective feed range of 1.04&amp;amp;ndash;1.45 GHz. A major focus of this work is the development of a standardized calibration pipeline for microquasar observations, including RFI mitigation, flux density, and polarization calibration, as well as multi-beam correlation inspections. Using On&amp;amp;ndash;Off mode and cross-beam verification, radio activity was detected in SS 433, GRS 1915+105 and Cyg X-3, while MAXI J1820+070 remained inactive. Both SS 433 and GRS 1915+105 show low linear polarization degrees of only a few percent. No credible quasi-periodic oscillations (QPOs) were detected in the 0.01&amp;amp;ndash;100 Hz range, suggesting that radio QPOs within this frequency range are relatively rare compared to those observed in the X-ray band. We therefore highlight the importance of future monitoring with high&amp;amp;ndash;time-resolution and high&amp;amp;ndash;sensitivity radio telescopes such as FAST, which will be crucial for revealing the correlation between jet and accretion processes and for uncovering the physical origin of QPOs.</p>
	]]></content:encoded>

	<dc:title>RadioObservations of Microquasars with FAST</dc:title>
			<dc:creator>Botao Li</dc:creator>
			<dc:creator>Wei Wang</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010006</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-03-06</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-03-06</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>6</prism:startingPage>
		<prism:doi>10.3390/astronomy5010006</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/5">

	<title>Astronomy, Vol. 5, Pages 5: Cosmological Viability of Linear and Power-Law Models in f(T,B,&amp;#120035;) Gravity Universe</title>
	<link>https://www.mdpi.com/2674-0346/5/1/5</link>
	<description>We investigate the cosmological implications of torsion&amp;amp;ndash;boundary gravity with explicit matter coupling in f(T,B,&amp;amp;#120035;) gravity. The purpose is to examine if such couplings offer observationally viable extensions to standard cosmology. Focusing on linear and power-law model realizations, we derive the modified Friedmann equations and analyze the resulting background dynamics. Using a combination of late-time datasets&amp;amp;mdash;including Cosmic Chronometers, Type Ia Supernovae, and Baryon Acoustic Oscillations&amp;amp;mdash;we perform a joint likelihood analysis to constrain the model parameters. Our results show that both f(T,B,&amp;amp;#120035;) models remain compatible with current observations and effectively reduce to the &amp;amp;Lambda;CDM paradigm in their appropriate parameter limits. While the power-law model exhibits mild dynamical deviations at intermediate redshifts, it remains statistically indistinguishable from the standard cosmological model. We conclude that f(T,B,&amp;amp;#120035;) gravity represents a viable and robust extension of torsional modified gravity, motivating further study of non-minimal matter&amp;amp;ndash;geometry couplings in cosmology.</description>
	<pubDate>2026-03-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 5: Cosmological Viability of Linear and Power-Law Models in f(T,B,&amp;#120035;) Gravity Universe</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/5">doi: 10.3390/astronomy5010005</a></p>
	<p>Authors:
		Yahia Al-Omar
		Majida Nahili
		Nidal Chamoun
		</p>
	<p>We investigate the cosmological implications of torsion&amp;amp;ndash;boundary gravity with explicit matter coupling in f(T,B,&amp;amp;#120035;) gravity. The purpose is to examine if such couplings offer observationally viable extensions to standard cosmology. Focusing on linear and power-law model realizations, we derive the modified Friedmann equations and analyze the resulting background dynamics. Using a combination of late-time datasets&amp;amp;mdash;including Cosmic Chronometers, Type Ia Supernovae, and Baryon Acoustic Oscillations&amp;amp;mdash;we perform a joint likelihood analysis to constrain the model parameters. Our results show that both f(T,B,&amp;amp;#120035;) models remain compatible with current observations and effectively reduce to the &amp;amp;Lambda;CDM paradigm in their appropriate parameter limits. While the power-law model exhibits mild dynamical deviations at intermediate redshifts, it remains statistically indistinguishable from the standard cosmological model. We conclude that f(T,B,&amp;amp;#120035;) gravity represents a viable and robust extension of torsional modified gravity, motivating further study of non-minimal matter&amp;amp;ndash;geometry couplings in cosmology.</p>
	]]></content:encoded>

	<dc:title>Cosmological Viability of Linear and Power-Law Models in f(T,B,&amp;amp;#120035;) Gravity Universe</dc:title>
			<dc:creator>Yahia Al-Omar</dc:creator>
			<dc:creator>Majida Nahili</dc:creator>
			<dc:creator>Nidal Chamoun</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010005</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-03-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-03-02</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>5</prism:startingPage>
		<prism:doi>10.3390/astronomy5010005</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/4">

	<title>Astronomy, Vol. 5, Pages 4: A Small Patch Hypothesis in Cosmology</title>
	<link>https://www.mdpi.com/2674-0346/5/1/4</link>
	<description>If our observable Universe is only a tiny region of a vastly larger and conformally older spacetime, then the usual formulations of the classical flatness and horizon problems of the Hot Big Bang can be reinterpreted as artifacts manifesting an observational selection effect; we occupy a small causal domain of a much larger causally-connected and possibly non-flat spacetime. A sufficiently large positive cosmological constant, &amp;amp;Lambda;, sets the future asymptotic horizon scale of the observable Universe, &amp;amp;sim;&amp;amp;Lambda;&amp;amp;minus;1/2, thereby implying that the observable Universe may simply be a minute patch of a far larger pre-existing one, hereafter a Small Patch Hypothesis. Importantly, this observational bound is purely geometric; regardless of when the Universe is observed, the maximum accessible scale is finite and fixed by &amp;amp;Lambda;, independent of inflationary dynamics, anthropic arguments, or assumptions about the global hosting spacetime. The externally possibly frozen past-eternal state implied by a pre-existing, causally connected spacetime motivates, but does not strictly require, viewing the perturbation field as being in (or arbitrarily close to) a coarse-grained maximum-entropy&amp;amp;mdash;equilibrium&amp;amp;mdash;configuration. Conditionalizing only on fixed mean and variance, a Gaussian distribution uniquely emerges, while the absence of entropy gradients corresponds to adiabaticity. In this work these features are therefore treated as plausible maximum-ignorance priors for super-horizon perturbations, rather than as rigorously derived consequences of a fully developed microscopic notion of gravitational entropy. In this sense, inflation becomes one viable realization of the proposed Small Patch Hypothesis. Here, one particular non-inflationary alternative is considered for illustrative purposes in which a primordial spectrum P&amp;amp;zeta;(k) of the gauge-invariant perturbation &amp;amp;zeta; that pre-dates the Big Bang grows logarithmically toward large scales, k&amp;amp;rarr;0, and in fact diverges at some finite kc. If kc&amp;amp;#8810;&amp;amp;Lambda;&amp;amp;minus;1/2, then our local cosmic patch probes only the regime where &amp;amp;zeta;&amp;amp;#8810;1 and appears exceptionally smooth. Over the comparatively narrow observable window, this P&amp;amp;zeta;(k) mimics a slightly red-tilted, inflation-like spectrum. Rather than introducing high-energy new fields, this perspective frames large-scale homogeneity, isotropy, Gaussianity, adiabaticity, and the observed thermodynamic Arrow of Time as possible consequences of restricted observational access to a much larger Universe in equilibrium, rather than signatures of a unique early-Universe mechanism. Current observations cannot distinguish this logarithmically running spectrum from the standard power-law one, but future probes&amp;amp;mdash;for example high-resolution 21-cm measurements of the Dark Ages&amp;amp;mdash;may be able to falsify it.</description>
	<pubDate>2026-02-09</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 4: A Small Patch Hypothesis in Cosmology</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/4">doi: 10.3390/astronomy5010004</a></p>
	<p>Authors:
		Meir Shimon
		</p>
	<p>If our observable Universe is only a tiny region of a vastly larger and conformally older spacetime, then the usual formulations of the classical flatness and horizon problems of the Hot Big Bang can be reinterpreted as artifacts manifesting an observational selection effect; we occupy a small causal domain of a much larger causally-connected and possibly non-flat spacetime. A sufficiently large positive cosmological constant, &amp;amp;Lambda;, sets the future asymptotic horizon scale of the observable Universe, &amp;amp;sim;&amp;amp;Lambda;&amp;amp;minus;1/2, thereby implying that the observable Universe may simply be a minute patch of a far larger pre-existing one, hereafter a Small Patch Hypothesis. Importantly, this observational bound is purely geometric; regardless of when the Universe is observed, the maximum accessible scale is finite and fixed by &amp;amp;Lambda;, independent of inflationary dynamics, anthropic arguments, or assumptions about the global hosting spacetime. The externally possibly frozen past-eternal state implied by a pre-existing, causally connected spacetime motivates, but does not strictly require, viewing the perturbation field as being in (or arbitrarily close to) a coarse-grained maximum-entropy&amp;amp;mdash;equilibrium&amp;amp;mdash;configuration. Conditionalizing only on fixed mean and variance, a Gaussian distribution uniquely emerges, while the absence of entropy gradients corresponds to adiabaticity. In this work these features are therefore treated as plausible maximum-ignorance priors for super-horizon perturbations, rather than as rigorously derived consequences of a fully developed microscopic notion of gravitational entropy. In this sense, inflation becomes one viable realization of the proposed Small Patch Hypothesis. Here, one particular non-inflationary alternative is considered for illustrative purposes in which a primordial spectrum P&amp;amp;zeta;(k) of the gauge-invariant perturbation &amp;amp;zeta; that pre-dates the Big Bang grows logarithmically toward large scales, k&amp;amp;rarr;0, and in fact diverges at some finite kc. If kc&amp;amp;#8810;&amp;amp;Lambda;&amp;amp;minus;1/2, then our local cosmic patch probes only the regime where &amp;amp;zeta;&amp;amp;#8810;1 and appears exceptionally smooth. Over the comparatively narrow observable window, this P&amp;amp;zeta;(k) mimics a slightly red-tilted, inflation-like spectrum. Rather than introducing high-energy new fields, this perspective frames large-scale homogeneity, isotropy, Gaussianity, adiabaticity, and the observed thermodynamic Arrow of Time as possible consequences of restricted observational access to a much larger Universe in equilibrium, rather than signatures of a unique early-Universe mechanism. Current observations cannot distinguish this logarithmically running spectrum from the standard power-law one, but future probes&amp;amp;mdash;for example high-resolution 21-cm measurements of the Dark Ages&amp;amp;mdash;may be able to falsify it.</p>
	]]></content:encoded>

	<dc:title>A Small Patch Hypothesis in Cosmology</dc:title>
			<dc:creator>Meir Shimon</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010004</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-02-09</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-02-09</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/astronomy5010004</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/3">

	<title>Astronomy, Vol. 5, Pages 3: Orbital Parameters and Planetary Radius of 55 Cancri e from TESS Data</title>
	<link>https://www.mdpi.com/2674-0346/5/1/3</link>
	<description>A large number of transits have been observed by TESS from the rapidly orbiting exoplanet 55 Cancri e. This amount of transit data, combined with the relatively high frequency of TESS observations, allows for a direct measurement of not only the planetary radius and orbital parameters but also the limb darkening coefficients of the host star. We obtain a planetary radius of 1.64&amp;amp;plusmn;0.10 earth radii, an orbital radius of 0.019&amp;amp;plusmn;0.009 AU, and an orbital inclination of 85&amp;amp;plusmn;17 degrees. For the quadratic limb darkening coefficients u1 and u2 we report measurements of u1=0.58&amp;amp;plusmn;0.48 and u2=0.64&amp;amp;plusmn;0.55, and discuss strategies to reduce the uncertainty in the measurement. We also measured the curvature of the transit depth as a function of time using an effective parametrization I&amp;amp;prime;(t)=C(t2), and found C=0.28&amp;amp;plusmn;0.03 in units of relative intensity per day squared. This parametrization resulted in a higher goodness-of-fit value than the quadratic model, with a reduced &amp;amp;chi;2 of 1.153 rather than 1.201 for the quadratic model, and a &amp;amp;Delta;BIC of 31.75 in favor of the effective parametrization.</description>
	<pubDate>2026-02-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 3: Orbital Parameters and Planetary Radius of 55 Cancri e from TESS Data</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/3">doi: 10.3390/astronomy5010003</a></p>
	<p>Authors:
		David Joffe
		Matt Bonvissuto
		</p>
	<p>A large number of transits have been observed by TESS from the rapidly orbiting exoplanet 55 Cancri e. This amount of transit data, combined with the relatively high frequency of TESS observations, allows for a direct measurement of not only the planetary radius and orbital parameters but also the limb darkening coefficients of the host star. We obtain a planetary radius of 1.64&amp;amp;plusmn;0.10 earth radii, an orbital radius of 0.019&amp;amp;plusmn;0.009 AU, and an orbital inclination of 85&amp;amp;plusmn;17 degrees. For the quadratic limb darkening coefficients u1 and u2 we report measurements of u1=0.58&amp;amp;plusmn;0.48 and u2=0.64&amp;amp;plusmn;0.55, and discuss strategies to reduce the uncertainty in the measurement. We also measured the curvature of the transit depth as a function of time using an effective parametrization I&amp;amp;prime;(t)=C(t2), and found C=0.28&amp;amp;plusmn;0.03 in units of relative intensity per day squared. This parametrization resulted in a higher goodness-of-fit value than the quadratic model, with a reduced &amp;amp;chi;2 of 1.153 rather than 1.201 for the quadratic model, and a &amp;amp;Delta;BIC of 31.75 in favor of the effective parametrization.</p>
	]]></content:encoded>

	<dc:title>Orbital Parameters and Planetary Radius of 55 Cancri e from TESS Data</dc:title>
			<dc:creator>David Joffe</dc:creator>
			<dc:creator>Matt Bonvissuto</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010003</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-02-06</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-02-06</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/astronomy5010003</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/2">

	<title>Astronomy, Vol. 5, Pages 2: Detailed Analysis of the Dynamics of Two Point Masses Under Gravitational Interaction</title>
	<link>https://www.mdpi.com/2674-0346/5/1/2</link>
	<description>The dynamics of two point masses interacting in a gravitational field has been the object of several scientific works. However, the complete explicit solution of the two-body problem is, to the best of our knowledge, not always available in the scientific literature. In this work, we describe the dynamics of a two-body system with that of an equivalent single-body with a reduced mass. Then, we solve the specific problems for elliptical, circular and parabolic trajectories, starting from different initial conditions. Through detailed analytical calculations, we write the Cartesian equations of the trajectories and the equations of motion both in the reference system of the centre of mass and in the original reference system. The proposed methodology is a simple but rigorous way to analyse the two-body dynamics under gravitational interactions, and can be applied also to more complex cases, such as the motion in a perturbed Newtonian potential and/or precession problems. The treatment presented in this work is particularly suitable to undergraduate students.</description>
	<pubDate>2026-01-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 2: Detailed Analysis of the Dynamics of Two Point Masses Under Gravitational Interaction</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/2">doi: 10.3390/astronomy5010002</a></p>
	<p>Authors:
		Luigi Sirignano
		Pierluigi Sirignano
		Roberto Guarino
		</p>
	<p>The dynamics of two point masses interacting in a gravitational field has been the object of several scientific works. However, the complete explicit solution of the two-body problem is, to the best of our knowledge, not always available in the scientific literature. In this work, we describe the dynamics of a two-body system with that of an equivalent single-body with a reduced mass. Then, we solve the specific problems for elliptical, circular and parabolic trajectories, starting from different initial conditions. Through detailed analytical calculations, we write the Cartesian equations of the trajectories and the equations of motion both in the reference system of the centre of mass and in the original reference system. The proposed methodology is a simple but rigorous way to analyse the two-body dynamics under gravitational interactions, and can be applied also to more complex cases, such as the motion in a perturbed Newtonian potential and/or precession problems. The treatment presented in this work is particularly suitable to undergraduate students.</p>
	]]></content:encoded>

	<dc:title>Detailed Analysis of the Dynamics of Two Point Masses Under Gravitational Interaction</dc:title>
			<dc:creator>Luigi Sirignano</dc:creator>
			<dc:creator>Pierluigi Sirignano</dc:creator>
			<dc:creator>Roberto Guarino</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010002</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2026-01-21</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2026-01-21</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/astronomy5010002</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/5/1/1">

	<title>Astronomy, Vol. 5, Pages 1: Jupiter Mass Binary Objects Show a Minimum Acceleration</title>
	<link>https://www.mdpi.com/2674-0346/5/1/1</link>
	<description>Forty-two Jupiter Mass Binary Objects (JuMBOs) have been discovered in the Trapezium Cluster: either brown dwarf stars or planets mutually orbiting in pairs. Here it is shown that, just as in galaxies and wide binaries, the mutual orbits of the objects in each of these twin systems deviate from the Newtonian and level off around a mutual acceleration of 2c2/&amp;amp;Theta;=2&amp;amp;times;10&amp;amp;minus;10 m/s2 supporting the minimum acceleration predicted by Quantised Inertia (QI), a theory that attributes inertial mass to an interaction between information horizons and quantum fields and predicts galaxy rotation without the need for dark matter. QI further predicts that the JuMBOs with separations of 400 AU should show orbital anomalies of 70 m/s. This could be tested using spectral Doppler data.</description>
	<pubDate>2025-12-26</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 5, Pages 1: Jupiter Mass Binary Objects Show a Minimum Acceleration</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/5/1/1">doi: 10.3390/astronomy5010001</a></p>
	<p>Authors:
		Michael E. McCulloch
		</p>
	<p>Forty-two Jupiter Mass Binary Objects (JuMBOs) have been discovered in the Trapezium Cluster: either brown dwarf stars or planets mutually orbiting in pairs. Here it is shown that, just as in galaxies and wide binaries, the mutual orbits of the objects in each of these twin systems deviate from the Newtonian and level off around a mutual acceleration of 2c2/&amp;amp;Theta;=2&amp;amp;times;10&amp;amp;minus;10 m/s2 supporting the minimum acceleration predicted by Quantised Inertia (QI), a theory that attributes inertial mass to an interaction between information horizons and quantum fields and predicts galaxy rotation without the need for dark matter. QI further predicts that the JuMBOs with separations of 400 AU should show orbital anomalies of 70 m/s. This could be tested using spectral Doppler data.</p>
	]]></content:encoded>

	<dc:title>Jupiter Mass Binary Objects Show a Minimum Acceleration</dc:title>
			<dc:creator>Michael E. McCulloch</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy5010001</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-12-26</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-12-26</prism:publicationDate>
	<prism:volume>5</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Brief Report</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/astronomy5010001</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/5/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/26">

	<title>Astronomy, Vol. 4, Pages 26: Chandra Observations of the X-Ray Binary Population in the Field of the Dwarf Galaxy IC 10</title>
	<link>https://www.mdpi.com/2674-0346/4/4/26</link>
	<description>IC 10 is a dwarf galaxy in Cassiopeia, located at a distance of 660 kpc, and hosts a young stellar population, a large number of Wolf&amp;amp;ndash;Rayet stars, and a large number of massive stars in general. Utilizing a series of 11 Chandra observations (spanning 2003&amp;amp;ndash;2021, with a total exposure of 235.1 ks), 375 point sources of X-ray emission were detected. Similar studies have been conducted earlier in the central region of IC 10. Here, we consider all regions covered by Chandra-ACIS. By comparing our catalog of X-ray sources with a published optical catalog, we found that 146 sources have optical counterparts. We also created a list of 60 blue supergiant (SG) candidates with X-ray binary (XRB) companions by using an optical color&amp;amp;ndash;magnitude selection criterion to isolate the blue SGs. Blue SG-XRBs form a major class of progenitors of double-degenerate binaries. Hence, their numbers are an important factor in modeling the rate of gravitational-wave sources. Identifying the nature of individual sources is necessary as it paves the way toward a comprehensive census of XRBs in IC 10, thus enabling meaningful comparisons with other Local Group galaxies exhibiting starbursts, such as the Magellanic Clouds.</description>
	<pubDate>2025-12-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 26: Chandra Observations of the X-Ray Binary Population in the Field of the Dwarf Galaxy IC 10</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/26">doi: 10.3390/astronomy4040026</a></p>
	<p>Authors:
		Sayantan Bhattacharya
		Silas G. T. Laycock
		Breanna A. Binder
		Dimitris M. Christodoulou
		</p>
	<p>IC 10 is a dwarf galaxy in Cassiopeia, located at a distance of 660 kpc, and hosts a young stellar population, a large number of Wolf&amp;amp;ndash;Rayet stars, and a large number of massive stars in general. Utilizing a series of 11 Chandra observations (spanning 2003&amp;amp;ndash;2021, with a total exposure of 235.1 ks), 375 point sources of X-ray emission were detected. Similar studies have been conducted earlier in the central region of IC 10. Here, we consider all regions covered by Chandra-ACIS. By comparing our catalog of X-ray sources with a published optical catalog, we found that 146 sources have optical counterparts. We also created a list of 60 blue supergiant (SG) candidates with X-ray binary (XRB) companions by using an optical color&amp;amp;ndash;magnitude selection criterion to isolate the blue SGs. Blue SG-XRBs form a major class of progenitors of double-degenerate binaries. Hence, their numbers are an important factor in modeling the rate of gravitational-wave sources. Identifying the nature of individual sources is necessary as it paves the way toward a comprehensive census of XRBs in IC 10, thus enabling meaningful comparisons with other Local Group galaxies exhibiting starbursts, such as the Magellanic Clouds.</p>
	]]></content:encoded>

	<dc:title>Chandra Observations of the X-Ray Binary Population in the Field of the Dwarf Galaxy IC 10</dc:title>
			<dc:creator>Sayantan Bhattacharya</dc:creator>
			<dc:creator>Silas G. T. Laycock</dc:creator>
			<dc:creator>Breanna A. Binder</dc:creator>
			<dc:creator>Dimitris M. Christodoulou</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040026</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-12-13</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-12-13</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>26</prism:startingPage>
		<prism:doi>10.3390/astronomy4040026</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/26</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/25">

	<title>Astronomy, Vol. 4, Pages 25: Disentangling the Cosmic/Comoving Duality: The Cognitive Stability and Typicality Tests</title>
	<link>https://www.mdpi.com/2674-0346/4/4/25</link>
	<description>Cosmological scenarios wherein the cumulative number of spontaneously formed, cognitively impaired, disembodied transient observers is vastly larger than the corresponding number of atypical &amp;amp;lsquo;ordinary observers&amp;amp;rsquo; (OOs) formed in the conventional way&amp;amp;mdash;essentially via cosmic evolution and gravitational instability&amp;amp;mdash;are disqualified in modern cosmology on the grounds of Cognitive Instability&amp;amp;mdash;the untrustworsiness of one own&amp;amp;rsquo;s reasoning&amp;amp;mdash;let alone the atypicality of OOs like us. According to the concordance &amp;amp;Lambda;CDM cosmological model&amp;amp;mdash;when described in the (expanding) &amp;amp;lsquo;cosmic frame&amp;amp;rsquo;&amp;amp;mdash;the cosmological expansion is future-eternal. In this frame we are atypical OOs, which are vastly outnumbered by typical Boltzmann Brains (BBs) that spontaneously form via sheer thermal fluctuations in the future-eternal asymptotic de Sitter spacetime. In the case that dark energy (DE) ultimately decays, the cumulative number of transient &amp;amp;lsquo;Freak Observers&amp;amp;rsquo; (FOs) formed and destroyed spontaneously by virtue of the quantum uncertainty principle ultimately overwhelms that of OOs. Either possibility is unacceptable. We argue that these unsettling conclusions are artifacts of employing the (default) cosmic frame description in which space expands. When analyzed in the comoving frame, OOs overwhelmingly outnumber both BBs and FOs. This suggests that the dual comoving description is the cognitively stable preferred framework for describing our evolving Universe. In this frame, space is globally static, masses monotonically increase, and the space describing gravitationally bounded objects monotonically contracts.</description>
	<pubDate>2025-12-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 25: Disentangling the Cosmic/Comoving Duality: The Cognitive Stability and Typicality Tests</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/25">doi: 10.3390/astronomy4040025</a></p>
	<p>Authors:
		Meir Shimon
		</p>
	<p>Cosmological scenarios wherein the cumulative number of spontaneously formed, cognitively impaired, disembodied transient observers is vastly larger than the corresponding number of atypical &amp;amp;lsquo;ordinary observers&amp;amp;rsquo; (OOs) formed in the conventional way&amp;amp;mdash;essentially via cosmic evolution and gravitational instability&amp;amp;mdash;are disqualified in modern cosmology on the grounds of Cognitive Instability&amp;amp;mdash;the untrustworsiness of one own&amp;amp;rsquo;s reasoning&amp;amp;mdash;let alone the atypicality of OOs like us. According to the concordance &amp;amp;Lambda;CDM cosmological model&amp;amp;mdash;when described in the (expanding) &amp;amp;lsquo;cosmic frame&amp;amp;rsquo;&amp;amp;mdash;the cosmological expansion is future-eternal. In this frame we are atypical OOs, which are vastly outnumbered by typical Boltzmann Brains (BBs) that spontaneously form via sheer thermal fluctuations in the future-eternal asymptotic de Sitter spacetime. In the case that dark energy (DE) ultimately decays, the cumulative number of transient &amp;amp;lsquo;Freak Observers&amp;amp;rsquo; (FOs) formed and destroyed spontaneously by virtue of the quantum uncertainty principle ultimately overwhelms that of OOs. Either possibility is unacceptable. We argue that these unsettling conclusions are artifacts of employing the (default) cosmic frame description in which space expands. When analyzed in the comoving frame, OOs overwhelmingly outnumber both BBs and FOs. This suggests that the dual comoving description is the cognitively stable preferred framework for describing our evolving Universe. In this frame, space is globally static, masses monotonically increase, and the space describing gravitationally bounded objects monotonically contracts.</p>
	]]></content:encoded>

	<dc:title>Disentangling the Cosmic/Comoving Duality: The Cognitive Stability and Typicality Tests</dc:title>
			<dc:creator>Meir Shimon</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040025</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-12-08</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-12-08</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>25</prism:startingPage>
		<prism:doi>10.3390/astronomy4040025</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/25</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/24">

	<title>Astronomy, Vol. 4, Pages 24: Constraints on the Hubble and Matter Density Parameters with and Without Modelling the CMB Anisotropies</title>
	<link>https://www.mdpi.com/2674-0346/4/4/24</link>
	<description>We consider constraints on the Hubble parameter H0 and the matter density parameter &amp;amp;Omega;M from the following: (i) the age of the Universe based on old stars and stellar populations in the Galactic disc and halo; (ii) the turnover scale in the matter power spectrum, which tells us the cosmological horizon at the epoch of matter-radiation equality; and (iii) the shape of the expansion history from supernovae (SNe) and baryon acoustic oscillations (BAOs) with no absolute calibration of either, a technique known as uncalibrated cosmic standards (UCS). A narrow region is consistent with all three constraints just outside their 1&amp;amp;sigma; uncertainties. Although this region is defined by techniques unrelated to the physics of recombination and the sound horizon then, the standard Planck fit to the CMB anisotropies falls precisely in this region. This concordance argues against early-time explanations for the anomalously high local estimate of H0 (the &amp;amp;lsquo;Hubble tension&amp;amp;rsquo;), which can only be reconciled with the age constraint at an implausibly low &amp;amp;Omega;M. We suggest instead that outflow from the local KBC supervoid inflates redshifts in the nearby universe and, thus, the apparent local H0. Given the difficulties with solutions in the early universe, we argue that the most promising alternative to a local void is a modification to the expansion history at late times, perhaps due to a changing dark energy density.</description>
	<pubDate>2025-11-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 24: Constraints on the Hubble and Matter Density Parameters with and Without Modelling the CMB Anisotropies</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/24">doi: 10.3390/astronomy4040024</a></p>
	<p>Authors:
		Indranil Banik
		Nick Samaras
		</p>
	<p>We consider constraints on the Hubble parameter H0 and the matter density parameter &amp;amp;Omega;M from the following: (i) the age of the Universe based on old stars and stellar populations in the Galactic disc and halo; (ii) the turnover scale in the matter power spectrum, which tells us the cosmological horizon at the epoch of matter-radiation equality; and (iii) the shape of the expansion history from supernovae (SNe) and baryon acoustic oscillations (BAOs) with no absolute calibration of either, a technique known as uncalibrated cosmic standards (UCS). A narrow region is consistent with all three constraints just outside their 1&amp;amp;sigma; uncertainties. Although this region is defined by techniques unrelated to the physics of recombination and the sound horizon then, the standard Planck fit to the CMB anisotropies falls precisely in this region. This concordance argues against early-time explanations for the anomalously high local estimate of H0 (the &amp;amp;lsquo;Hubble tension&amp;amp;rsquo;), which can only be reconciled with the age constraint at an implausibly low &amp;amp;Omega;M. We suggest instead that outflow from the local KBC supervoid inflates redshifts in the nearby universe and, thus, the apparent local H0. Given the difficulties with solutions in the early universe, we argue that the most promising alternative to a local void is a modification to the expansion history at late times, perhaps due to a changing dark energy density.</p>
	]]></content:encoded>

	<dc:title>Constraints on the Hubble and Matter Density Parameters with and Without Modelling the CMB Anisotropies</dc:title>
			<dc:creator>Indranil Banik</dc:creator>
			<dc:creator>Nick Samaras</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040024</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-11-19</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-11-19</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>24</prism:startingPage>
		<prism:doi>10.3390/astronomy4040024</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/24</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/23">

	<title>Astronomy, Vol. 4, Pages 23: Solar Flare Forecast: A Comparative Analysis of Machine Learning Algorithms for Predicting Solar Flare Classes</title>
	<link>https://www.mdpi.com/2674-0346/4/4/23</link>
	<description>Solar flares are among the most powerful and dynamic events in the solar system, resulting from the sudden release of magnetic energy stored in the Sun&amp;amp;rsquo;s atmosphere. These energetic bursts of electromagnetic radiation can release up to 1032 erg of energy, impacting space weather and posing risks to technological infrastructure and therefore require accurate forecasting of solar flare occurrences and intensities. This study evaluates the predictive performance of three machine learning algorithms&amp;amp;mdash;Random Forest (RF), k-Nearest Neighbors (kNN), and Extreme Gradient Boosting (XGBoost)&amp;amp;mdash;for classifying solar flares into four categories (B, C, M, X). Using 13 parameters of the SHARP dataset, the effectiveness of the models was evaluated in binary and multiclass classification tasks. The analysis utilized 8 principal components (PCs), capturing 95% of data variance, and 100 PCs, capturing 97.5% of variance. Our approach uniquely combines binary and multiclass classification with different levels of dimensionality reduction, an innovative methodology not previously explored in the context of solar flare prediction. Employing a 10-fold stratified cross-validation and grid search for hyperparameter tuning ensured robust model evaluation. Our findings indicate that RF and XGBoost consistently demonstrate strong performance across all metrics, benefiting significantly from increased dimensionality. The insights of this study enhance future research by optimizing dimensionality reduction techniques and informing model selection for astrophysical tasks. By integrating this newly acquired knowledge into future research, more accurate space weather forecasting systems can be developed, along with a deeper understanding of solar physics.</description>
	<pubDate>2025-11-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 23: Solar Flare Forecast: A Comparative Analysis of Machine Learning Algorithms for Predicting Solar Flare Classes</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/23">doi: 10.3390/astronomy4040023</a></p>
	<p>Authors:
		Julia Bringewald
		Olivier Parisot
		</p>
	<p>Solar flares are among the most powerful and dynamic events in the solar system, resulting from the sudden release of magnetic energy stored in the Sun&amp;amp;rsquo;s atmosphere. These energetic bursts of electromagnetic radiation can release up to 1032 erg of energy, impacting space weather and posing risks to technological infrastructure and therefore require accurate forecasting of solar flare occurrences and intensities. This study evaluates the predictive performance of three machine learning algorithms&amp;amp;mdash;Random Forest (RF), k-Nearest Neighbors (kNN), and Extreme Gradient Boosting (XGBoost)&amp;amp;mdash;for classifying solar flares into four categories (B, C, M, X). Using 13 parameters of the SHARP dataset, the effectiveness of the models was evaluated in binary and multiclass classification tasks. The analysis utilized 8 principal components (PCs), capturing 95% of data variance, and 100 PCs, capturing 97.5% of variance. Our approach uniquely combines binary and multiclass classification with different levels of dimensionality reduction, an innovative methodology not previously explored in the context of solar flare prediction. Employing a 10-fold stratified cross-validation and grid search for hyperparameter tuning ensured robust model evaluation. Our findings indicate that RF and XGBoost consistently demonstrate strong performance across all metrics, benefiting significantly from increased dimensionality. The insights of this study enhance future research by optimizing dimensionality reduction techniques and informing model selection for astrophysical tasks. By integrating this newly acquired knowledge into future research, more accurate space weather forecasting systems can be developed, along with a deeper understanding of solar physics.</p>
	]]></content:encoded>

	<dc:title>Solar Flare Forecast: A Comparative Analysis of Machine Learning Algorithms for Predicting Solar Flare Classes</dc:title>
			<dc:creator>Julia Bringewald</dc:creator>
			<dc:creator>Olivier Parisot</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040023</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-11-13</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-11-13</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>23</prism:startingPage>
		<prism:doi>10.3390/astronomy4040023</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/23</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/22">

	<title>Astronomy, Vol. 4, Pages 22: A Study of Four Distinct Photonic Crystal Fibers for the Maximization of the Optical Hawking Effect in Analog Models of the Event Horizon</title>
	<link>https://www.mdpi.com/2674-0346/4/4/22</link>
	<description>This work aims to maximize the Hawking emission temperature arising in the optical analog model of the event horizon of an astrophysical black hole. A weak probe wave interacts with an intense ultrashort optical pulse via the Kerr effect in a photonic crystal fiber. This interaction causes the probe wave to experience an effective spacetime geometry characterized by the presence of an optical event horizon, where the analogous Hawking radiation effect arises. Here we refer to the simulated or classical version of the analog of Hawking radiation. This study considers four distinct types of photonic crystal fibers with anomalous dispersion curves that allow for maximizing the effect. Our first three numerical simulations indicate that a Hawking emission temperature of up to 361 K can be achieved with a photonic crystal fiber with two zero-dispersion wavelengths, while the emission temperature values in the original investigation are lower than 244 K. And in the fourth, we can see that we have a configuration in which the temperature can be improved up to 1027 K. Moreover, these results also emphasize the feasibility of using analog models to test the quantum effects of gravity, such as Hawking radiation produced by typical black holes, whose magnitude is far below the temperature of the cosmic microwave background (2.7 K).</description>
	<pubDate>2025-11-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 22: A Study of Four Distinct Photonic Crystal Fibers for the Maximization of the Optical Hawking Effect in Analog Models of the Event Horizon</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/22">doi: 10.3390/astronomy4040022</a></p>
	<p>Authors:
		Alfonso González Jiménez
		Enderson Falcón Gómez
		Isabel Carnoto Amat
		Luis Enrique García Muñoz
		</p>
	<p>This work aims to maximize the Hawking emission temperature arising in the optical analog model of the event horizon of an astrophysical black hole. A weak probe wave interacts with an intense ultrashort optical pulse via the Kerr effect in a photonic crystal fiber. This interaction causes the probe wave to experience an effective spacetime geometry characterized by the presence of an optical event horizon, where the analogous Hawking radiation effect arises. Here we refer to the simulated or classical version of the analog of Hawking radiation. This study considers four distinct types of photonic crystal fibers with anomalous dispersion curves that allow for maximizing the effect. Our first three numerical simulations indicate that a Hawking emission temperature of up to 361 K can be achieved with a photonic crystal fiber with two zero-dispersion wavelengths, while the emission temperature values in the original investigation are lower than 244 K. And in the fourth, we can see that we have a configuration in which the temperature can be improved up to 1027 K. Moreover, these results also emphasize the feasibility of using analog models to test the quantum effects of gravity, such as Hawking radiation produced by typical black holes, whose magnitude is far below the temperature of the cosmic microwave background (2.7 K).</p>
	]]></content:encoded>

	<dc:title>A Study of Four Distinct Photonic Crystal Fibers for the Maximization of the Optical Hawking Effect in Analog Models of the Event Horizon</dc:title>
			<dc:creator>Alfonso González Jiménez</dc:creator>
			<dc:creator>Enderson Falcón Gómez</dc:creator>
			<dc:creator>Isabel Carnoto Amat</dc:creator>
			<dc:creator>Luis Enrique García Muñoz</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040022</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-11-10</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-11-10</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>22</prism:startingPage>
		<prism:doi>10.3390/astronomy4040022</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/22</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/21">

	<title>Astronomy, Vol. 4, Pages 21: General Relativistic Effect on Sitnikov Three-Body Problem: Restricted Case</title>
	<link>https://www.mdpi.com/2674-0346/4/4/21</link>
	<description>We investigate the effect of general relativity on the Sitnikov problem. The Sitnikov problem is one of the simplest three-body problems, in which the two primary bodies (a binary system) have equal mass m and orbit their barycenter, while the third body is treated as a test particle under Newtonian gravity. The trajectory of the test particle is perpendicular to the orbital plane of the binary (along z-axis) and passes through the barycenter of the two primaries. To study the general relativistic contributions, we first derive the equations of motion for both the binary and the test particle based on the first post-Newtonian Einstein&amp;amp;ndash;Infeld&amp;amp;ndash;Hoffmann equation, and integrate these equations numerically. We examine the behavior of the test particle (third body) as a function of the orbital eccentricity of the central binary e, the dimensionless gravitational radius &amp;amp;lambda;, which characterizes the strength of general relativistic effect, and the initial position of the test particle z&amp;amp;macr;0. Our numerical calculations reveal the following; as general relativistic effects &amp;amp;lambda; increase and the eccentricity e of the binary orbit grows, the distance r&amp;amp;macr; between the test particle and the primary star undergoes complicated oscillations over time. Consequently, the gravitational force acting on the test particle also varies in a complex manner. This leads to a resonance state between the position z&amp;amp;macr; of the test particle and the distance r&amp;amp;macr;, causing the energy E of the test particle to become E&amp;amp;ge;0. This triggers the effective ejection of the test particle due to the gravitational slingshot effect. In this paper, we shall refer to this ejection mechanism of test particle as the &amp;amp;ldquo;Sitnikov mechanism.&amp;amp;rdquo; As a concrete phenomenon that becomes noticeable, the increase in general relativistic effects and the eccentricity of the binary orbit leads to the following: (a) ejection of test particles from the system in a shorter time, and (b) increasing escape velocity of the test particle from the system. As an astrophysical application, we point out that the high-velocity ejection of test particles induced by the Sitnikov mechanism could contribute to elucidating the formation processes of astrophysical jets and hyper-velocity stars.</description>
	<pubDate>2025-11-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 21: General Relativistic Effect on Sitnikov Three-Body Problem: Restricted Case</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/21">doi: 10.3390/astronomy4040021</a></p>
	<p>Authors:
		Hideyoshi Arakida
		</p>
	<p>We investigate the effect of general relativity on the Sitnikov problem. The Sitnikov problem is one of the simplest three-body problems, in which the two primary bodies (a binary system) have equal mass m and orbit their barycenter, while the third body is treated as a test particle under Newtonian gravity. The trajectory of the test particle is perpendicular to the orbital plane of the binary (along z-axis) and passes through the barycenter of the two primaries. To study the general relativistic contributions, we first derive the equations of motion for both the binary and the test particle based on the first post-Newtonian Einstein&amp;amp;ndash;Infeld&amp;amp;ndash;Hoffmann equation, and integrate these equations numerically. We examine the behavior of the test particle (third body) as a function of the orbital eccentricity of the central binary e, the dimensionless gravitational radius &amp;amp;lambda;, which characterizes the strength of general relativistic effect, and the initial position of the test particle z&amp;amp;macr;0. Our numerical calculations reveal the following; as general relativistic effects &amp;amp;lambda; increase and the eccentricity e of the binary orbit grows, the distance r&amp;amp;macr; between the test particle and the primary star undergoes complicated oscillations over time. Consequently, the gravitational force acting on the test particle also varies in a complex manner. This leads to a resonance state between the position z&amp;amp;macr; of the test particle and the distance r&amp;amp;macr;, causing the energy E of the test particle to become E&amp;amp;ge;0. This triggers the effective ejection of the test particle due to the gravitational slingshot effect. In this paper, we shall refer to this ejection mechanism of test particle as the &amp;amp;ldquo;Sitnikov mechanism.&amp;amp;rdquo; As a concrete phenomenon that becomes noticeable, the increase in general relativistic effects and the eccentricity of the binary orbit leads to the following: (a) ejection of test particles from the system in a shorter time, and (b) increasing escape velocity of the test particle from the system. As an astrophysical application, we point out that the high-velocity ejection of test particles induced by the Sitnikov mechanism could contribute to elucidating the formation processes of astrophysical jets and hyper-velocity stars.</p>
	]]></content:encoded>

	<dc:title>General Relativistic Effect on Sitnikov Three-Body Problem: Restricted Case</dc:title>
			<dc:creator>Hideyoshi Arakida</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040021</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-11-03</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-11-03</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>21</prism:startingPage>
		<prism:doi>10.3390/astronomy4040021</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/21</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/20">

	<title>Astronomy, Vol. 4, Pages 20: A Census of Chemically Peculiar Stars in Stellar Associations</title>
	<link>https://www.mdpi.com/2674-0346/4/4/20</link>
	<description>The pre-main-sequence evolution of the chemically peculiar (CP) stars on the upper main sequence is still a vast mystery and not well understood. Our analysis of young associations and open clusters aims to find (very) young CP stars to try to put a lower boundary on the age of such objects. Using three catalogues of open clusters and associations, we determined membership probabilities using HDBSCAN. The hot stars from this selection were submitted to synthetic &amp;amp;Delta;a photometry, spectral, and light curve classification to determine which ones are CP stars and candidates. Subsequently, we used spectral energy distribution fitting and emission line analysis to check for possible PMS CP stars. The results were compared to the literature. We detected 971 CP stars and candidates in 217 clusters and associations. A relatively large fraction, &amp;amp;sim;10% of those, show characteristics of PMS CP stars. This significantly expands the known list of candidate PMS CP stars, bringing us closer to solving the mystery of their origin.</description>
	<pubDate>2025-10-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 20: A Census of Chemically Peculiar Stars in Stellar Associations</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/20">doi: 10.3390/astronomy4040020</a></p>
	<p>Authors:
		Lukas Kueß
		Ernst Paunzen
		</p>
	<p>The pre-main-sequence evolution of the chemically peculiar (CP) stars on the upper main sequence is still a vast mystery and not well understood. Our analysis of young associations and open clusters aims to find (very) young CP stars to try to put a lower boundary on the age of such objects. Using three catalogues of open clusters and associations, we determined membership probabilities using HDBSCAN. The hot stars from this selection were submitted to synthetic &amp;amp;Delta;a photometry, spectral, and light curve classification to determine which ones are CP stars and candidates. Subsequently, we used spectral energy distribution fitting and emission line analysis to check for possible PMS CP stars. The results were compared to the literature. We detected 971 CP stars and candidates in 217 clusters and associations. A relatively large fraction, &amp;amp;sim;10% of those, show characteristics of PMS CP stars. This significantly expands the known list of candidate PMS CP stars, bringing us closer to solving the mystery of their origin.</p>
	]]></content:encoded>

	<dc:title>A Census of Chemically Peculiar Stars in Stellar Associations</dc:title>
			<dc:creator>Lukas Kueß</dc:creator>
			<dc:creator>Ernst Paunzen</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040020</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-10-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-10-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>20</prism:startingPage>
		<prism:doi>10.3390/astronomy4040020</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/19">

	<title>Astronomy, Vol. 4, Pages 19: Time Markers for SETI in Binary Systems: History and Prospects</title>
	<link>https://www.mdpi.com/2674-0346/4/4/19</link>
	<description>Contemporary surveys in the search for extraterrestrial intelligence (SETI) typically make one-off &amp;amp;ldquo;spot scans&amp;amp;rdquo; across the sky to search planetary systems for narrow-band radio signals that would indicate the presence of intelligent life. Spot scans may span a duration of seconds to minutes in order to observe a large number of targets with limited resources, but such a strategy does not necessarily consider the timing of exactly when to listen for extraterrestrial signals. Several ideas for possible time markers were suggested in the first few decades of SETI, such as the use of recurrent supernovae, gamma ray bursts, or pulsars as a way of establishing directionality and attracting attention toward an extraterrestrial beacon. Civilizations in binary systems might even choose the points of periastron and apastron in its host system to send transmissions to other single-star civilizations. However, all of these timing considerations were developed prior to the age of exoplanets, which enables a more detailed assessment of targets suitable for SETI. This paper suggests SETI strategies for circumbinary and circumprimary planets based upon the timing of orbital events in such systems. Events such as orbital extremes could represent a logical time marker for extraterrestrial civilizations to transmit, if they desire to be detected. Likewise, a transiting binary pair with inhabited planets around each star could yield maximum detectability of leakage radiation when both stars eclipse within our field of view. As planets in binary systems continue to be discovered, limited-duration SETI surveys should selectively target such systems based upon the occurrence of reasonable time markers.</description>
	<pubDate>2025-10-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 19: Time Markers for SETI in Binary Systems: History and Prospects</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/19">doi: 10.3390/astronomy4040019</a></p>
	<p>Authors:
		Jacob Haqq-Misra
		</p>
	<p>Contemporary surveys in the search for extraterrestrial intelligence (SETI) typically make one-off &amp;amp;ldquo;spot scans&amp;amp;rdquo; across the sky to search planetary systems for narrow-band radio signals that would indicate the presence of intelligent life. Spot scans may span a duration of seconds to minutes in order to observe a large number of targets with limited resources, but such a strategy does not necessarily consider the timing of exactly when to listen for extraterrestrial signals. Several ideas for possible time markers were suggested in the first few decades of SETI, such as the use of recurrent supernovae, gamma ray bursts, or pulsars as a way of establishing directionality and attracting attention toward an extraterrestrial beacon. Civilizations in binary systems might even choose the points of periastron and apastron in its host system to send transmissions to other single-star civilizations. However, all of these timing considerations were developed prior to the age of exoplanets, which enables a more detailed assessment of targets suitable for SETI. This paper suggests SETI strategies for circumbinary and circumprimary planets based upon the timing of orbital events in such systems. Events such as orbital extremes could represent a logical time marker for extraterrestrial civilizations to transmit, if they desire to be detected. Likewise, a transiting binary pair with inhabited planets around each star could yield maximum detectability of leakage radiation when both stars eclipse within our field of view. As planets in binary systems continue to be discovered, limited-duration SETI surveys should selectively target such systems based upon the occurrence of reasonable time markers.</p>
	]]></content:encoded>

	<dc:title>Time Markers for SETI in Binary Systems: History and Prospects</dc:title>
			<dc:creator>Jacob Haqq-Misra</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040019</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-10-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-10-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>19</prism:startingPage>
		<prism:doi>10.3390/astronomy4040019</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/4/18">

	<title>Astronomy, Vol. 4, Pages 18: On the Possible Nature of White Holes</title>
	<link>https://www.mdpi.com/2674-0346/4/4/18</link>
	<description>This paper considers non-singular black holes. It discusses the observation of particles falling onto ordinary and non-singular black holes from the perspective of a distant observer. It is demonstrated that, during a stage in the evolution of non-singular black holes, powerful energy fluxes can be emitted. Distant observers may interpret these fluxes as white holes.</description>
	<pubDate>2025-10-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 18: On the Possible Nature of White Holes</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/4/18">doi: 10.3390/astronomy4040018</a></p>
	<p>Authors:
		Mikhail Pekker
		Mikhail N. Shneider
		</p>
	<p>This paper considers non-singular black holes. It discusses the observation of particles falling onto ordinary and non-singular black holes from the perspective of a distant observer. It is demonstrated that, during a stage in the evolution of non-singular black holes, powerful energy fluxes can be emitted. Distant observers may interpret these fluxes as white holes.</p>
	]]></content:encoded>

	<dc:title>On the Possible Nature of White Holes</dc:title>
			<dc:creator>Mikhail Pekker</dc:creator>
			<dc:creator>Mikhail N. Shneider</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4040018</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-10-10</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-10-10</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>18</prism:startingPage>
		<prism:doi>10.3390/astronomy4040018</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/4/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/17">

	<title>Astronomy, Vol. 4, Pages 17: Cosmic-Ray Boosted Diffuse Supernova Neutrinos</title>
	<link>https://www.mdpi.com/2674-0346/4/3/17</link>
	<description>The subject of boosted fluxes of dark matter or cosmic relic neutrinos via scattering on cosmic rays has received considerable attention recently. This article investigates the boosted neutrino flux from the scattering of cosmic rays and the so-far undetected diffuse supernova neutrino background, taking into account both galactic and extragalactic cosmic rays. The calculated flux is many orders of magnitude smaller than either the galactic diffuse neutrino emission, the extragalactic astrophysical flux measured by IceCube, or the cosmogenic neutrino flux expected at the highest energies.</description>
	<pubDate>2025-09-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 17: Cosmic-Ray Boosted Diffuse Supernova Neutrinos</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/17">doi: 10.3390/astronomy4030017</a></p>
	<p>Authors:
		Alexander Sandrock
		</p>
	<p>The subject of boosted fluxes of dark matter or cosmic relic neutrinos via scattering on cosmic rays has received considerable attention recently. This article investigates the boosted neutrino flux from the scattering of cosmic rays and the so-far undetected diffuse supernova neutrino background, taking into account both galactic and extragalactic cosmic rays. The calculated flux is many orders of magnitude smaller than either the galactic diffuse neutrino emission, the extragalactic astrophysical flux measured by IceCube, or the cosmogenic neutrino flux expected at the highest energies.</p>
	]]></content:encoded>

	<dc:title>Cosmic-Ray Boosted Diffuse Supernova Neutrinos</dc:title>
			<dc:creator>Alexander Sandrock</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030017</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-09-12</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-09-12</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>17</prism:startingPage>
		<prism:doi>10.3390/astronomy4030017</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/16">

	<title>Astronomy, Vol. 4, Pages 16: Extending the Quantum Memory Matrix to Dark Energy: Residual Vacuum Imprint and Slow-Roll Entropy Fields</title>
	<link>https://www.mdpi.com/2674-0346/4/3/16</link>
	<description>We extend the Quantum Memory Matrix (QMM) framework&amp;amp;mdash;previously shown to unify gauge interactions and reproduce cold dark matter phenomenology&amp;amp;mdash;to account for the observed late-time cosmic acceleration. In QMM, each Planck-scale cell carries a finite-dimensional Hilbert space of quantum imprints. We show that (1) once local unitary evolution saturates the available micro-states, a uniform residual &amp;amp;ldquo;vacuum-imprint energy&amp;amp;rdquo; remains; its stress&amp;amp;ndash;energy tensor is of pure cosmological-constant form, with magnitude suppressed by the cell capacity, naturally yielding &amp;amp;rho;&amp;amp;Lambda;&amp;amp;#8771;(2&amp;amp;times;10&amp;amp;minus;3eV)4; and (2) if imprint writes continue but are overdamped by cosmic expansion, the coarse-grained entropy field S(t) undergoes slow-roll evolution, generating an effective equation of state w(z)&amp;amp;asymp;&amp;amp;minus;1+O(10&amp;amp;minus;2) that is testable by DESI, Euclid, and Roman. We derive the modified Friedmann equations, linear perturbations, and joint constraints from Planck 2018, BAO, and Pantheon +, finding that the QMM imprint model reproduces the observed TT, TE, and EE spectra without introducing additional free parameters and alleviates the H0 tension while remaining consistent with the large-scale structure. In this picture, dark matter and dark energy arise as gradient-dominated and potential-dominated limits of the same underlying information field, completing the QMM cosmological sector with predictive power and internal consistency.</description>
	<pubDate>2025-09-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 16: Extending the Quantum Memory Matrix to Dark Energy: Residual Vacuum Imprint and Slow-Roll Entropy Fields</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/16">doi: 10.3390/astronomy4030016</a></p>
	<p>Authors:
		Florian Neukart
		Eike Marx
		Valerii Vinokur
		</p>
	<p>We extend the Quantum Memory Matrix (QMM) framework&amp;amp;mdash;previously shown to unify gauge interactions and reproduce cold dark matter phenomenology&amp;amp;mdash;to account for the observed late-time cosmic acceleration. In QMM, each Planck-scale cell carries a finite-dimensional Hilbert space of quantum imprints. We show that (1) once local unitary evolution saturates the available micro-states, a uniform residual &amp;amp;ldquo;vacuum-imprint energy&amp;amp;rdquo; remains; its stress&amp;amp;ndash;energy tensor is of pure cosmological-constant form, with magnitude suppressed by the cell capacity, naturally yielding &amp;amp;rho;&amp;amp;Lambda;&amp;amp;#8771;(2&amp;amp;times;10&amp;amp;minus;3eV)4; and (2) if imprint writes continue but are overdamped by cosmic expansion, the coarse-grained entropy field S(t) undergoes slow-roll evolution, generating an effective equation of state w(z)&amp;amp;asymp;&amp;amp;minus;1+O(10&amp;amp;minus;2) that is testable by DESI, Euclid, and Roman. We derive the modified Friedmann equations, linear perturbations, and joint constraints from Planck 2018, BAO, and Pantheon +, finding that the QMM imprint model reproduces the observed TT, TE, and EE spectra without introducing additional free parameters and alleviates the H0 tension while remaining consistent with the large-scale structure. In this picture, dark matter and dark energy arise as gradient-dominated and potential-dominated limits of the same underlying information field, completing the QMM cosmological sector with predictive power and internal consistency.</p>
	]]></content:encoded>

	<dc:title>Extending the Quantum Memory Matrix to Dark Energy: Residual Vacuum Imprint and Slow-Roll Entropy Fields</dc:title>
			<dc:creator>Florian Neukart</dc:creator>
			<dc:creator>Eike Marx</dc:creator>
			<dc:creator>Valerii Vinokur</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030016</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-09-10</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-09-10</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>16</prism:startingPage>
		<prism:doi>10.3390/astronomy4030016</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/15">

	<title>Astronomy, Vol. 4, Pages 15: The Status of the Astrophysical Parameters of Upper Main Sequence Stars</title>
	<link>https://www.mdpi.com/2674-0346/4/3/15</link>
	<description>Calibrating the ages, masses, and radii of stars on the upper main sequence depends heavily on accurate measurements of the effective temperature (Teff) and surface gravity (logg). These parameters are difficult to obtain meticulously due to the nature of hot stars, which exhibit features such as rapid rotation, atomic diffusion, pulsation, and stellar winds. We compare the Teff and logg values of apparent normal B-F stars in four recent catalogues that employ different methods and pipelines to obtain these parameters. We derived various statistical parameters to compare the differences between the catalogues and discussed the astrophysical implications of these differences. Our results show that the huge differences in Teff (up to 104 K) and logg (up to 2 dex) between the catalogues have serious implications on the determination of ages, masses, and radii of the stars in question. We conclude that there appears to be no homogeneous set of stellar parameters on the upper main sequence, and one must be cautious when interpreting results obtained from using only one of the catalogues. The homogenisation of said parameters is an essential task for the future and will have a significant impact on astrophysical research dealing with stars on the upper main sequence.</description>
	<pubDate>2025-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 15: The Status of the Astrophysical Parameters of Upper Main Sequence Stars</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/15">doi: 10.3390/astronomy4030015</a></p>
	<p>Authors:
		Lukas Kueß
		Ernst Paunzen
		</p>
	<p>Calibrating the ages, masses, and radii of stars on the upper main sequence depends heavily on accurate measurements of the effective temperature (Teff) and surface gravity (logg). These parameters are difficult to obtain meticulously due to the nature of hot stars, which exhibit features such as rapid rotation, atomic diffusion, pulsation, and stellar winds. We compare the Teff and logg values of apparent normal B-F stars in four recent catalogues that employ different methods and pipelines to obtain these parameters. We derived various statistical parameters to compare the differences between the catalogues and discussed the astrophysical implications of these differences. Our results show that the huge differences in Teff (up to 104 K) and logg (up to 2 dex) between the catalogues have serious implications on the determination of ages, masses, and radii of the stars in question. We conclude that there appears to be no homogeneous set of stellar parameters on the upper main sequence, and one must be cautious when interpreting results obtained from using only one of the catalogues. The homogenisation of said parameters is an essential task for the future and will have a significant impact on astrophysical research dealing with stars on the upper main sequence.</p>
	]]></content:encoded>

	<dc:title>The Status of the Astrophysical Parameters of Upper Main Sequence Stars</dc:title>
			<dc:creator>Lukas Kueß</dc:creator>
			<dc:creator>Ernst Paunzen</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030015</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-08-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/astronomy4030015</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/14">

	<title>Astronomy, Vol. 4, Pages 14: Gravity Wave Phase Shift in a Cold Quark Star with a Nonconvex QCD BZT Shock Wave Van Der Waals Equation of State</title>
	<link>https://www.mdpi.com/2674-0346/4/3/14</link>
	<description>We investigate BZT shocks and the QCD phase transition in the dense core of a cold quark star in beta equilibrium subject to the multicomponent van der Waals (MvdW) equation of state (EoS) as a model of internal structure. When this system is expressed in terms of multiple components, it can be used to explore the impact of a phase transition from a hadronic state to a quark plasma state with a complex clustering structure. The clustering can take the form of colored diquarks or triquarks and bound colorless meson, baryon, or hyperon states at the phase transition boundary. The resulting multicomponent EoS system is nonconvex, which can give rise to Bethe&amp;amp;ndash;Zel&amp;amp;rsquo;dovich&amp;amp;ndash;Thompson (BZT) phase-changing shock waves. Using the BZT shock wave condition, we find constraints on the quark density and examine how this changes the tidal deformability of the compact core. These results are then combined with the TOV equations to find the resulting mass and radius relationship. These states are compared to recent astrophysical high-mass neutron star systems, which may provide evidence for a core that has undergone a quark gluon phase transition such as PSR 0943+10 or GW 190814.</description>
	<pubDate>2025-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 14: Gravity Wave Phase Shift in a Cold Quark Star with a Nonconvex QCD BZT Shock Wave Van Der Waals Equation of State</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/14">doi: 10.3390/astronomy4030014</a></p>
	<p>Authors:
		Keith Andrew
		Eric V. Steinfelds
		Kristopher A. Andrew
		</p>
	<p>We investigate BZT shocks and the QCD phase transition in the dense core of a cold quark star in beta equilibrium subject to the multicomponent van der Waals (MvdW) equation of state (EoS) as a model of internal structure. When this system is expressed in terms of multiple components, it can be used to explore the impact of a phase transition from a hadronic state to a quark plasma state with a complex clustering structure. The clustering can take the form of colored diquarks or triquarks and bound colorless meson, baryon, or hyperon states at the phase transition boundary. The resulting multicomponent EoS system is nonconvex, which can give rise to Bethe&amp;amp;ndash;Zel&amp;amp;rsquo;dovich&amp;amp;ndash;Thompson (BZT) phase-changing shock waves. Using the BZT shock wave condition, we find constraints on the quark density and examine how this changes the tidal deformability of the compact core. These results are then combined with the TOV equations to find the resulting mass and radius relationship. These states are compared to recent astrophysical high-mass neutron star systems, which may provide evidence for a core that has undergone a quark gluon phase transition such as PSR 0943+10 or GW 190814.</p>
	]]></content:encoded>

	<dc:title>Gravity Wave Phase Shift in a Cold Quark Star with a Nonconvex QCD BZT Shock Wave Van Der Waals Equation of State</dc:title>
			<dc:creator>Keith Andrew</dc:creator>
			<dc:creator>Eric V. Steinfelds</dc:creator>
			<dc:creator>Kristopher A. Andrew</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030014</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-08-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/astronomy4030014</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/13">

	<title>Astronomy, Vol. 4, Pages 13: The Use of Conditional Variational Autoencoders in Generating Stellar Spectra</title>
	<link>https://www.mdpi.com/2674-0346/4/3/13</link>
	<description>We present a conditional variational autoencoder (CVAE) that generates stellar spectra covering 4000 &amp;amp;le; Teff &amp;amp;le; 11,000 K, 2.0&amp;amp;le;logg&amp;amp;le;5.0 dex, &amp;amp;minus;1.5&amp;amp;le;[M/H]&amp;amp;le;+1.5 dex, vsini&amp;amp;le;300 km/s, &amp;amp;xi;t between 0 and 4 km/s, and for any instrumental resolving powers less than 115,000. The spectra can be calculated in the wavelength range 4450&amp;amp;ndash;5400 &amp;amp;Aring;. Trained on a grid of SYNSPEC spectra, the network synthesizes a spectrum in around two orders of magnitude faster than line-by-line radiative transfer. We validate the CVAE on 104 test spectra unseen during training. Pixel-wise statistics yield a median absolute residual of &amp;amp;lt;1.8&amp;amp;times;10&amp;amp;minus;3 flux units with no wavelength-dependent bias. A residual error map across the parameters plane shows &amp;amp;#10216;|&amp;amp;Delta;F|&amp;amp;#10217;&amp;amp;lt;2&amp;amp;times;10&amp;amp;minus;3 everywhere, and marginal diagnostics versus Teff, logg, vesini, &amp;amp;xi;t, and [M/H] reveal no relevant trends. These results demonstrate that the CVAE can serve as a drop-in, physics-aware surrogate for radiative transfer codes, enabling real-time forward modeling in stellar parameter inference and offering promising tools for spectra synthesis for large astrophysical data analysis.</description>
	<pubDate>2025-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 13: The Use of Conditional Variational Autoencoders in Generating Stellar Spectra</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/13">doi: 10.3390/astronomy4030013</a></p>
	<p>Authors:
		Marwan Gebran
		Ian Bentley
		</p>
	<p>We present a conditional variational autoencoder (CVAE) that generates stellar spectra covering 4000 &amp;amp;le; Teff &amp;amp;le; 11,000 K, 2.0&amp;amp;le;logg&amp;amp;le;5.0 dex, &amp;amp;minus;1.5&amp;amp;le;[M/H]&amp;amp;le;+1.5 dex, vsini&amp;amp;le;300 km/s, &amp;amp;xi;t between 0 and 4 km/s, and for any instrumental resolving powers less than 115,000. The spectra can be calculated in the wavelength range 4450&amp;amp;ndash;5400 &amp;amp;Aring;. Trained on a grid of SYNSPEC spectra, the network synthesizes a spectrum in around two orders of magnitude faster than line-by-line radiative transfer. We validate the CVAE on 104 test spectra unseen during training. Pixel-wise statistics yield a median absolute residual of &amp;amp;lt;1.8&amp;amp;times;10&amp;amp;minus;3 flux units with no wavelength-dependent bias. A residual error map across the parameters plane shows &amp;amp;#10216;|&amp;amp;Delta;F|&amp;amp;#10217;&amp;amp;lt;2&amp;amp;times;10&amp;amp;minus;3 everywhere, and marginal diagnostics versus Teff, logg, vesini, &amp;amp;xi;t, and [M/H] reveal no relevant trends. These results demonstrate that the CVAE can serve as a drop-in, physics-aware surrogate for radiative transfer codes, enabling real-time forward modeling in stellar parameter inference and offering promising tools for spectra synthesis for large astrophysical data analysis.</p>
	]]></content:encoded>

	<dc:title>The Use of Conditional Variational Autoencoders in Generating Stellar Spectra</dc:title>
			<dc:creator>Marwan Gebran</dc:creator>
			<dc:creator>Ian Bentley</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030013</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-08-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>13</prism:startingPage>
		<prism:doi>10.3390/astronomy4030013</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/12">

	<title>Astronomy, Vol. 4, Pages 12: Nonlinearity in Turbulent Diffusion as a Possible Cause of Stellar Flares</title>
	<link>https://www.mdpi.com/2674-0346/4/3/12</link>
	<description>Extremely powerful flares releasing energy well above 1032 erg are rare compared to the typical manifestations of solar activity, which are already being routinely monitored by the existing Space Weather network&amp;amp;mdash;with some level of predictability. However, much less is known about the mechanisms behind such rare events (like the well-documented Carrington event of 1859) or about hypothetical superflares that could exceed current energy estimates by several orders of magnitude. We propose a model based on the nonlinear suppression of turbulent diffusion with increasing magnetic field, which ultimately leads to the random occurrence of regions with a magnetic field amplitude significantly exceeding the magnetic field amplitude in a regular cycle. This is similar to the mechanism of a local &amp;amp;ldquo;explosion of an overheated boiler&amp;amp;rdquo;. Such regions can be correlated with flares. In our model, flares have different powers.</description>
	<pubDate>2025-07-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 12: Nonlinearity in Turbulent Diffusion as a Possible Cause of Stellar Flares</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/12">doi: 10.3390/astronomy4030012</a></p>
	<p>Authors:
		Elena Popova
		</p>
	<p>Extremely powerful flares releasing energy well above 1032 erg are rare compared to the typical manifestations of solar activity, which are already being routinely monitored by the existing Space Weather network&amp;amp;mdash;with some level of predictability. However, much less is known about the mechanisms behind such rare events (like the well-documented Carrington event of 1859) or about hypothetical superflares that could exceed current energy estimates by several orders of magnitude. We propose a model based on the nonlinear suppression of turbulent diffusion with increasing magnetic field, which ultimately leads to the random occurrence of regions with a magnetic field amplitude significantly exceeding the magnetic field amplitude in a regular cycle. This is similar to the mechanism of a local &amp;amp;ldquo;explosion of an overheated boiler&amp;amp;rdquo;. Such regions can be correlated with flares. In our model, flares have different powers.</p>
	]]></content:encoded>

	<dc:title>Nonlinearity in Turbulent Diffusion as a Possible Cause of Stellar Flares</dc:title>
			<dc:creator>Elena Popova</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030012</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-07-07</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-07-07</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>12</prism:startingPage>
		<prism:doi>10.3390/astronomy4030012</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/3/11">

	<title>Astronomy, Vol. 4, Pages 11: A Library of 77 Multibody Solar and Extrasolar Subsystems&amp;mdash;A Review of Their Dynamical Properties, Global Mean-Motion Resonances, and the Landau-Damped Mean Tidal Fields</title>
	<link>https://www.mdpi.com/2674-0346/4/3/11</link>
	<description>We revisit 77 relaxed (extra)solar multibody (sub)systems containing 2&amp;amp;ndash;9 bodies orbiting about gravitationally dominant central bodies. The listings are complete down to (sub)systems with 5 orbiting bodies and additionally contain 33 smaller systems with 2&amp;amp;ndash;4 orbiting bodies. Most of the multiplanet systems (68) have been observed outside of our solar system, and very few of them (5) exhibit classical Laplace resonances (LRs). The remaining 9 subsystems have been found in our solar system; they include 7 well-known satellite groups in addition to the four gaseous giant planets and the four terrestrial planets, and they exhibit only one classical Laplace resonant chain, the famous Galilean LR. The orbiting bodies (planets, dwarfs, or satellites) appear to be locked in/near global mean-motion resonances (MMRs), as these are determined in reference to the orbital period of the most massive (most inert) body in each (sub)system. We present a library of these 77 multibody subsystems for future use and reference. The library listings of dynamical properties also include regular spacings of the orbital semimajor axes. Regularities in the spatial configurations of the bodies were determined from patterns that had existed in the mean tidal field that drove multibody migrations toward MMRs, well before the tidal field was erased by the process of `gravitational Landau damping&amp;amp;rsquo; which concluded its work when all major bodies had finally settled in/near the global MMRs presently observed. Finally, detailed comparisons of results help us discern the longest commonly-occurring MMR chains, distinguish the most important groups of triple MMRs, and identify a new criterion for the absence of librations in triple MMRs.</description>
	<pubDate>2025-06-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 11: A Library of 77 Multibody Solar and Extrasolar Subsystems&amp;mdash;A Review of Their Dynamical Properties, Global Mean-Motion Resonances, and the Landau-Damped Mean Tidal Fields</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/3/11">doi: 10.3390/astronomy4030011</a></p>
	<p>Authors:
		Dimitris M. Christodoulou
		Silas G. T. Laycock
		Demosthenes Kazanas
		</p>
	<p>We revisit 77 relaxed (extra)solar multibody (sub)systems containing 2&amp;amp;ndash;9 bodies orbiting about gravitationally dominant central bodies. The listings are complete down to (sub)systems with 5 orbiting bodies and additionally contain 33 smaller systems with 2&amp;amp;ndash;4 orbiting bodies. Most of the multiplanet systems (68) have been observed outside of our solar system, and very few of them (5) exhibit classical Laplace resonances (LRs). The remaining 9 subsystems have been found in our solar system; they include 7 well-known satellite groups in addition to the four gaseous giant planets and the four terrestrial planets, and they exhibit only one classical Laplace resonant chain, the famous Galilean LR. The orbiting bodies (planets, dwarfs, or satellites) appear to be locked in/near global mean-motion resonances (MMRs), as these are determined in reference to the orbital period of the most massive (most inert) body in each (sub)system. We present a library of these 77 multibody subsystems for future use and reference. The library listings of dynamical properties also include regular spacings of the orbital semimajor axes. Regularities in the spatial configurations of the bodies were determined from patterns that had existed in the mean tidal field that drove multibody migrations toward MMRs, well before the tidal field was erased by the process of `gravitational Landau damping&amp;amp;rsquo; which concluded its work when all major bodies had finally settled in/near the global MMRs presently observed. Finally, detailed comparisons of results help us discern the longest commonly-occurring MMR chains, distinguish the most important groups of triple MMRs, and identify a new criterion for the absence of librations in triple MMRs.</p>
	]]></content:encoded>

	<dc:title>A Library of 77 Multibody Solar and Extrasolar Subsystems&amp;amp;mdash;A Review of Their Dynamical Properties, Global Mean-Motion Resonances, and the Landau-Damped Mean Tidal Fields</dc:title>
			<dc:creator>Dimitris M. Christodoulou</dc:creator>
			<dc:creator>Silas G. T. Laycock</dc:creator>
			<dc:creator>Demosthenes Kazanas</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4030011</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-06-23</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-06-23</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>11</prism:startingPage>
		<prism:doi>10.3390/astronomy4030011</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/3/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/2/10">

	<title>Astronomy, Vol. 4, Pages 10: Core&amp;ndash;Corona Decomposition of Very Compact (Neutron) Stars: Accounting for Current Data of XTE J1814-338</title>
	<link>https://www.mdpi.com/2674-0346/4/2/10</link>
	<description>A core&amp;amp;ndash;corona decomposition of compact (neutron) star models was compared with the current mass&amp;amp;ndash;radius data of the outlier XTE J1814-338. The corona (which may also be dubbed the envelope, halo or outer crust) is assumed to be of Standard Model matter, with an equation of state that is supposed to be faithfully known and accommodates nearly all other neutron star data. The core, solely parameterized by its mass, radius and transition pressure, presents a challenge regarding its composition. We derived a range of core parameters needed to describe the current data of XTE J1814-338.</description>
	<pubDate>2025-06-09</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 10: Core&amp;ndash;Corona Decomposition of Very Compact (Neutron) Stars: Accounting for Current Data of XTE J1814-338</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/2/10">doi: 10.3390/astronomy4020010</a></p>
	<p>Authors:
		Rico Zöllner
		Burkhard Kämpfer
		</p>
	<p>A core&amp;amp;ndash;corona decomposition of compact (neutron) star models was compared with the current mass&amp;amp;ndash;radius data of the outlier XTE J1814-338. The corona (which may also be dubbed the envelope, halo or outer crust) is assumed to be of Standard Model matter, with an equation of state that is supposed to be faithfully known and accommodates nearly all other neutron star data. The core, solely parameterized by its mass, radius and transition pressure, presents a challenge regarding its composition. We derived a range of core parameters needed to describe the current data of XTE J1814-338.</p>
	]]></content:encoded>

	<dc:title>Core&amp;amp;ndash;Corona Decomposition of Very Compact (Neutron) Stars: Accounting for Current Data of XTE J1814-338</dc:title>
			<dc:creator>Rico Zöllner</dc:creator>
			<dc:creator>Burkhard Kämpfer</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4020010</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-06-09</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-06-09</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>10</prism:startingPage>
		<prism:doi>10.3390/astronomy4020010</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/2/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/2/9">

	<title>Astronomy, Vol. 4, Pages 9: Analytic Investigation of the Imprints of Dark Energy and Charge on the Kerr&amp;ndash;Newmann&amp;ndash;De Sitter Black-Hole Photon Ring</title>
	<link>https://www.mdpi.com/2674-0346/4/2/9</link>
	<description>In 2019, the Event Horizon Telescope (EHT) released the first image of a black hole, sparking huge interest in the study of black-hole images. We present analytical solutions to the null geodesic equations for Kerr&amp;amp;ndash;Newman&amp;amp;ndash;de Sitter black holes derived using Jacobi elliptic functions. Using these solutions, we have performed an analytic ray-tracing simulation to model direct images, lensing rings, and photon rings, considering standard observers and zero angular momentum observers (ZAMOs). Additionally, we have derived analytic expressions for the critical parameters governing the structure of the photon ring and analyzed them in detail. From the foregoing, an increase in charge leads to a decrease in both time delay and Lyapunov exponent, while the change in azimuthal angle is insignificant. These findings improve our understanding of the effects of charge on black-hole photon rings and provide a foundation for future studies.</description>
	<pubDate>2025-05-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 9: Analytic Investigation of the Imprints of Dark Energy and Charge on the Kerr&amp;ndash;Newmann&amp;ndash;De Sitter Black-Hole Photon Ring</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/2/9">doi: 10.3390/astronomy4020009</a></p>
	<p>Authors:
		James Mugambi
		Eunice Omwoyo
		Dismas Wamalwa
		</p>
	<p>In 2019, the Event Horizon Telescope (EHT) released the first image of a black hole, sparking huge interest in the study of black-hole images. We present analytical solutions to the null geodesic equations for Kerr&amp;amp;ndash;Newman&amp;amp;ndash;de Sitter black holes derived using Jacobi elliptic functions. Using these solutions, we have performed an analytic ray-tracing simulation to model direct images, lensing rings, and photon rings, considering standard observers and zero angular momentum observers (ZAMOs). Additionally, we have derived analytic expressions for the critical parameters governing the structure of the photon ring and analyzed them in detail. From the foregoing, an increase in charge leads to a decrease in both time delay and Lyapunov exponent, while the change in azimuthal angle is insignificant. These findings improve our understanding of the effects of charge on black-hole photon rings and provide a foundation for future studies.</p>
	]]></content:encoded>

	<dc:title>Analytic Investigation of the Imprints of Dark Energy and Charge on the Kerr&amp;amp;ndash;Newmann&amp;amp;ndash;De Sitter Black-Hole Photon Ring</dc:title>
			<dc:creator>James Mugambi</dc:creator>
			<dc:creator>Eunice Omwoyo</dc:creator>
			<dc:creator>Dismas Wamalwa</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4020009</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-05-21</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-05-21</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>9</prism:startingPage>
		<prism:doi>10.3390/astronomy4020009</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/2/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/2/8">

	<title>Astronomy, Vol. 4, Pages 8: At the Edge of Uncertainty: Decoding the Cosmological Constant Value with the Bose&amp;ndash;Einstein Distribution</title>
	<link>https://www.mdpi.com/2674-0346/4/2/8</link>
	<description>We propose that the observed value of the cosmological constant may be explained by a fundamental uncertainty in the spacetime metric, which arises when combining the principle that mass and energy curve spacetime with the quantum uncertainty associated with particle localization. Since the position of a quantum particle cannot be sharply defined, the gravitational influence of such particles leads to intrinsic ambiguity in the formation of spacetime geometry. Recent experimental studies suggest that gravitational effects persist down to length scales of approximately 10&amp;amp;minus;5 m, while quantum coherence and macroscopic quantum phenomena such as Bose&amp;amp;ndash;Einstein condensation and superfluidity also manifest at similar scales. Motivated by these findings, we identify a length scale of spacetime uncertainty, LZ&amp;amp;sim;2.2&amp;amp;times;10&amp;amp;minus;5 m, which corresponds to the geometric mean of the Planck length and the radius of the observable universe. We argue that this intermediate scale may act as an effective cutoff in vacuum energy calculations. Furthermore, we explore the interpretation of dark energy as a Bose&amp;amp;ndash;Einstein distribution with a characteristic reduced wavelength matching this uncertainty scale. This approach provides a potential bridge between cosmological and quantum regimes and offers a phenomenologically motivated perspective on the cosmological constant problem.</description>
	<pubDate>2025-05-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 8: At the Edge of Uncertainty: Decoding the Cosmological Constant Value with the Bose&amp;ndash;Einstein Distribution</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/2/8">doi: 10.3390/astronomy4020008</a></p>
	<p>Authors:
		Ahmed Farag Ali
		Nader Inan
		</p>
	<p>We propose that the observed value of the cosmological constant may be explained by a fundamental uncertainty in the spacetime metric, which arises when combining the principle that mass and energy curve spacetime with the quantum uncertainty associated with particle localization. Since the position of a quantum particle cannot be sharply defined, the gravitational influence of such particles leads to intrinsic ambiguity in the formation of spacetime geometry. Recent experimental studies suggest that gravitational effects persist down to length scales of approximately 10&amp;amp;minus;5 m, while quantum coherence and macroscopic quantum phenomena such as Bose&amp;amp;ndash;Einstein condensation and superfluidity also manifest at similar scales. Motivated by these findings, we identify a length scale of spacetime uncertainty, LZ&amp;amp;sim;2.2&amp;amp;times;10&amp;amp;minus;5 m, which corresponds to the geometric mean of the Planck length and the radius of the observable universe. We argue that this intermediate scale may act as an effective cutoff in vacuum energy calculations. Furthermore, we explore the interpretation of dark energy as a Bose&amp;amp;ndash;Einstein distribution with a characteristic reduced wavelength matching this uncertainty scale. This approach provides a potential bridge between cosmological and quantum regimes and offers a phenomenologically motivated perspective on the cosmological constant problem.</p>
	]]></content:encoded>

	<dc:title>At the Edge of Uncertainty: Decoding the Cosmological Constant Value with the Bose&amp;amp;ndash;Einstein Distribution</dc:title>
			<dc:creator>Ahmed Farag Ali</dc:creator>
			<dc:creator>Nader Inan</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4020008</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-05-13</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-05-13</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>8</prism:startingPage>
		<prism:doi>10.3390/astronomy4020008</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/2/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/2/7">

	<title>Astronomy, Vol. 4, Pages 7: Hilbert Bundles and Holographic Space&amp;ndash;Time Models</title>
	<link>https://www.mdpi.com/2674-0346/4/2/7</link>
	<description>We reformulate holographic space&amp;amp;ndash;time models in terms of Hilbert bundles over the space of the time-like geodesics in a Lorentzian manifold. This reformulation resolves the issue of the action of non-compact isometry groups on finite-dimensional Hilbert spaces. Following Jacobson, I view the background geometry as a hydrodynamic flow, whose connection to an underlying quantum system follows from the Bekenstein&amp;amp;ndash;Hawking relation between area and entropy, generalized to arbitrary causal diamonds. The time-like geodesics are equivalent to the nested sequences of causal diamonds, and the area of the holoscreen (The holoscreen is the maximal d&amp;amp;minus;2 volume (&amp;amp;ldquo;area&amp;amp;rdquo;) leaf of a null foliation of the diamond boundary. I use the term area to refer to its volume.) encodes the entropy of a certain density matrix on a finite-dimensional Hilbert space. I review arguments that the modular Hamiltonian of a diamond is a cutoff version of the Virasoro generator L0 of a 1+1-dimensional CFT of a large central charge, living on an interval in the longitudinal coordinate on the diamond boundary. The cutoff is chosen so that the von Neumann entropy is lnD&amp;amp;#8900;, up to subleading corrections, in the limit of a large-dimension diamond Hilbert space. I also connect those arguments to the derivation of the &amp;amp;rsquo;t Hooft commutation relations for horizon fluctuations. I present a tentative connection between the &amp;amp;rsquo;t Hooft relations and U(1) currents in the CFTs on the past and future diamond boundaries. The &amp;amp;rsquo;t Hooft relations are related to the Schwinger term in the commutator of the vector and axial currents. The paper in can be read as evidence that the near-horizon dynamics for causal diamonds much larger than the Planck scale is equivalent to a topological field theory of the &amp;amp;rsquo;t Hooft CR plus small fluctuations in the transverse geometry. Connes&amp;amp;rsquo; demonstration that the Riemannian geometry is encoded in the Dirac operator leads one to a completely finite theory of transverse geometry fluctuations, in which the variables are fermionic generators of a superalgebra, which are the expansion coefficients of the sections of the spinor bundle in Dirac eigenfunctions. A finite cutoff on the Dirac spectrum gives rise to the area law for entropy and makes the geometry both &amp;amp;ldquo;fuzzy&amp;amp;rdquo; and quantum. Following the analysis of Carlip and Solodukhin, I model the expansion coefficients as two-dimensional fermionic fields. I argue that the local excitations in the interior of a diamond are constrained states where the spinor variables vanish in the regions of small area on the holoscreen. This leads to an argument that the quantum gravity in asymptotically flat space must be exactly supersymmetric.</description>
	<pubDate>2025-04-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 7: Hilbert Bundles and Holographic Space&amp;ndash;Time Models</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/2/7">doi: 10.3390/astronomy4020007</a></p>
	<p>Authors:
		Tom Banks
		</p>
	<p>We reformulate holographic space&amp;amp;ndash;time models in terms of Hilbert bundles over the space of the time-like geodesics in a Lorentzian manifold. This reformulation resolves the issue of the action of non-compact isometry groups on finite-dimensional Hilbert spaces. Following Jacobson, I view the background geometry as a hydrodynamic flow, whose connection to an underlying quantum system follows from the Bekenstein&amp;amp;ndash;Hawking relation between area and entropy, generalized to arbitrary causal diamonds. The time-like geodesics are equivalent to the nested sequences of causal diamonds, and the area of the holoscreen (The holoscreen is the maximal d&amp;amp;minus;2 volume (&amp;amp;ldquo;area&amp;amp;rdquo;) leaf of a null foliation of the diamond boundary. I use the term area to refer to its volume.) encodes the entropy of a certain density matrix on a finite-dimensional Hilbert space. I review arguments that the modular Hamiltonian of a diamond is a cutoff version of the Virasoro generator L0 of a 1+1-dimensional CFT of a large central charge, living on an interval in the longitudinal coordinate on the diamond boundary. The cutoff is chosen so that the von Neumann entropy is lnD&amp;amp;#8900;, up to subleading corrections, in the limit of a large-dimension diamond Hilbert space. I also connect those arguments to the derivation of the &amp;amp;rsquo;t Hooft commutation relations for horizon fluctuations. I present a tentative connection between the &amp;amp;rsquo;t Hooft relations and U(1) currents in the CFTs on the past and future diamond boundaries. The &amp;amp;rsquo;t Hooft relations are related to the Schwinger term in the commutator of the vector and axial currents. The paper in can be read as evidence that the near-horizon dynamics for causal diamonds much larger than the Planck scale is equivalent to a topological field theory of the &amp;amp;rsquo;t Hooft CR plus small fluctuations in the transverse geometry. Connes&amp;amp;rsquo; demonstration that the Riemannian geometry is encoded in the Dirac operator leads one to a completely finite theory of transverse geometry fluctuations, in which the variables are fermionic generators of a superalgebra, which are the expansion coefficients of the sections of the spinor bundle in Dirac eigenfunctions. A finite cutoff on the Dirac spectrum gives rise to the area law for entropy and makes the geometry both &amp;amp;ldquo;fuzzy&amp;amp;rdquo; and quantum. Following the analysis of Carlip and Solodukhin, I model the expansion coefficients as two-dimensional fermionic fields. I argue that the local excitations in the interior of a diamond are constrained states where the spinor variables vanish in the regions of small area on the holoscreen. This leads to an argument that the quantum gravity in asymptotically flat space must be exactly supersymmetric.</p>
	]]></content:encoded>

	<dc:title>Hilbert Bundles and Holographic Space&amp;amp;ndash;Time Models</dc:title>
			<dc:creator>Tom Banks</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4020007</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-04-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-04-22</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>7</prism:startingPage>
		<prism:doi>10.3390/astronomy4020007</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/2/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/2/6">

	<title>Astronomy, Vol. 4, Pages 6: Distance to M87 as the Mode of the Modulus Distribution</title>
	<link>https://www.mdpi.com/2674-0346/4/2/6</link>
	<description>de Grijs and Bono (ApJS 2020, 246, 3) compiled a list of distances to M87 from the literature published in the last 100 years. They reported the arithmetic mean of the three most stable tracers (Cepheids, tip of the red giant branch, and surface brightness fluctuations). The arithmetic mean is one of the measures of central tendency of a distribution; others are the median and mode. The three do not align for asymmetric distributions, which is the case for the distance moduli &amp;amp;mu;0 to M87. I construct a kernel density distribution of the set of &amp;amp;mu;0 and estimate the recommended distance to M87 as its mode, obtaining &amp;amp;mu;0=31.06&amp;amp;plusmn;0.001(statistical)&amp;amp;minus;0.06+0.04(systematic) mag, corresponding to D=16.29&amp;amp;minus;0.45+0.30 Mpc, which yields uncertainties smaller than those associated with the mean and median.</description>
	<pubDate>2025-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 6: Distance to M87 as the Mode of the Modulus Distribution</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/2/6">doi: 10.3390/astronomy4020006</a></p>
	<p>Authors:
		Mariusz Tarnopolski
		</p>
	<p>de Grijs and Bono (ApJS 2020, 246, 3) compiled a list of distances to M87 from the literature published in the last 100 years. They reported the arithmetic mean of the three most stable tracers (Cepheids, tip of the red giant branch, and surface brightness fluctuations). The arithmetic mean is one of the measures of central tendency of a distribution; others are the median and mode. The three do not align for asymmetric distributions, which is the case for the distance moduli &amp;amp;mu;0 to M87. I construct a kernel density distribution of the set of &amp;amp;mu;0 and estimate the recommended distance to M87 as its mode, obtaining &amp;amp;mu;0=31.06&amp;amp;plusmn;0.001(statistical)&amp;amp;minus;0.06+0.04(systematic) mag, corresponding to D=16.29&amp;amp;minus;0.45+0.30 Mpc, which yields uncertainties smaller than those associated with the mean and median.</p>
	]]></content:encoded>

	<dc:title>Distance to M87 as the Mode of the Modulus Distribution</dc:title>
			<dc:creator>Mariusz Tarnopolski</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4020006</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-04-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-04-02</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>6</prism:startingPage>
		<prism:doi>10.3390/astronomy4020006</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/2/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/1/5">

	<title>Astronomy, Vol. 4, Pages 5: Solar Particle Acceleration</title>
	<link>https://www.mdpi.com/2674-0346/4/1/5</link>
	<description>High-energy particles may be accelerated widely in stellar coronae; probably by the same processes we find in the Sun. Here, we have learned of two physical mechanisms that dominate the acceleration of solar energetic particles (SEPs). The highest energies and intensities are produced in &amp;amp;ldquo;gradual&amp;amp;rdquo; events where shock waves are driven from the Sun by fast and wide coronal mass ejections (CMEs). Smaller, but more numerous &amp;amp;ldquo;impulsive&amp;amp;rdquo; events with unusual particle compositions are produced during magnetic reconnection in solar jets and flares. Jets provide open magnetic field lines where SEPs can escape. Closed magnetic loops contain this energy to produce bright, hot flares; perhaps even contributing to heating the low corona in profuse nanoflares. Streaming protons amplify Alfv&amp;amp;eacute;n waves upstream of the shocks. These waves scatter and trap SEPs and, in large events, modify the element abundances and flatten the low-energy spectra upstream. Shocks also re-accelerate the residual ions from earlier impulsive events, when available, that characteristically dominate the energetic heavy-ion abundances. The large CME-driven shock waves develop an extremely wide longitudinal span, filling much of the inner heliosphere with energetic particles.</description>
	<pubDate>2025-03-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 5: Solar Particle Acceleration</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/1/5">doi: 10.3390/astronomy4010005</a></p>
	<p>Authors:
		Donald V. Reames
		</p>
	<p>High-energy particles may be accelerated widely in stellar coronae; probably by the same processes we find in the Sun. Here, we have learned of two physical mechanisms that dominate the acceleration of solar energetic particles (SEPs). The highest energies and intensities are produced in &amp;amp;ldquo;gradual&amp;amp;rdquo; events where shock waves are driven from the Sun by fast and wide coronal mass ejections (CMEs). Smaller, but more numerous &amp;amp;ldquo;impulsive&amp;amp;rdquo; events with unusual particle compositions are produced during magnetic reconnection in solar jets and flares. Jets provide open magnetic field lines where SEPs can escape. Closed magnetic loops contain this energy to produce bright, hot flares; perhaps even contributing to heating the low corona in profuse nanoflares. Streaming protons amplify Alfv&amp;amp;eacute;n waves upstream of the shocks. These waves scatter and trap SEPs and, in large events, modify the element abundances and flatten the low-energy spectra upstream. Shocks also re-accelerate the residual ions from earlier impulsive events, when available, that characteristically dominate the energetic heavy-ion abundances. The large CME-driven shock waves develop an extremely wide longitudinal span, filling much of the inner heliosphere with energetic particles.</p>
	]]></content:encoded>

	<dc:title>Solar Particle Acceleration</dc:title>
			<dc:creator>Donald V. Reames</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4010005</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-03-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-03-18</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>5</prism:startingPage>
		<prism:doi>10.3390/astronomy4010005</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/1/4">

	<title>Astronomy, Vol. 4, Pages 4: Deciphering the Electron Spectral Hardening in AMS-02</title>
	<link>https://www.mdpi.com/2674-0346/4/1/4</link>
	<description>We analyze the electron cosmic-ray spectrum from AMS-02, focusing on the spectral hardening around 42 GeV. Our findings confirm that this feature is intrinsic to the primary electron component rather than a byproduct of contamination from primary positron sources. Even under conservative assumptions, its significance remains at about 7&amp;amp;sigma;, strongly indicating a genuine spectral break. Accordingly, we introduce a new, more realistic parametric fit, which we recommend for the next round of AMS-02 analyses. Once the sources of systematic uncertainties are better constrained, this refined approach can either reinforce or refute our conclusions, providing a clearer understanding of the observed electron spectrum. If confirmed, we propose that this hardening most likely arises from interstellar transport or acceleration effects.</description>
	<pubDate>2025-02-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 4: Deciphering the Electron Spectral Hardening in AMS-02</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/1/4">doi: 10.3390/astronomy4010004</a></p>
	<p>Authors:
		Carmelo Evoli
		</p>
	<p>We analyze the electron cosmic-ray spectrum from AMS-02, focusing on the spectral hardening around 42 GeV. Our findings confirm that this feature is intrinsic to the primary electron component rather than a byproduct of contamination from primary positron sources. Even under conservative assumptions, its significance remains at about 7&amp;amp;sigma;, strongly indicating a genuine spectral break. Accordingly, we introduce a new, more realistic parametric fit, which we recommend for the next round of AMS-02 analyses. Once the sources of systematic uncertainties are better constrained, this refined approach can either reinforce or refute our conclusions, providing a clearer understanding of the observed electron spectrum. If confirmed, we propose that this hardening most likely arises from interstellar transport or acceleration effects.</p>
	]]></content:encoded>

	<dc:title>Deciphering the Electron Spectral Hardening in AMS-02</dc:title>
			<dc:creator>Carmelo Evoli</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4010004</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-02-28</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-02-28</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>4</prism:startingPage>
		<prism:doi>10.3390/astronomy4010004</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/1/3">

	<title>Astronomy, Vol. 4, Pages 3: Line Ratio in the C-like Ion Spectrum O III: Testing Atomic Theory Predictions Through the Observation of Galaxies</title>
	<link>https://www.mdpi.com/2674-0346/4/1/3</link>
	<description>The progress made in atomic structure computations has indicated that certain line ratios of forbidden transitions may be slightly different from earlier assumptions. In order to check this theory, we evaluate previous observations of dwarf galaxies by the UVES spectrograph at the VLT telescope on ESO Paranal for the line ratios of branched decays in C-like oxygen ions [O III] that are insensitive to the local environment. Our findings show that the observed line ratio for [O III] (r=3.005&amp;amp;plusmn;0.237) aligns with recent theoretical predictions based on more sophisticated models, while it deviates from older computations. Additionally, the analysis of line profiles suggests that, in some cases, the spectral resolution was insufficient to fully resolve dynamic substructures within the galaxies. Our results emphasize the importance of improved data quality and consistency for future studies, especially for future searches of finestructure constant variations at higher redshifts using this method.</description>
	<pubDate>2025-02-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 3: Line Ratio in the C-like Ion Spectrum O III: Testing Atomic Theory Predictions Through the Observation of Galaxies</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/1/3">doi: 10.3390/astronomy4010003</a></p>
	<p>Authors:
		Julius Richard Dreisbach
		Dominik J. Bomans
		Elmar Träbert
		</p>
	<p>The progress made in atomic structure computations has indicated that certain line ratios of forbidden transitions may be slightly different from earlier assumptions. In order to check this theory, we evaluate previous observations of dwarf galaxies by the UVES spectrograph at the VLT telescope on ESO Paranal for the line ratios of branched decays in C-like oxygen ions [O III] that are insensitive to the local environment. Our findings show that the observed line ratio for [O III] (r=3.005&amp;amp;plusmn;0.237) aligns with recent theoretical predictions based on more sophisticated models, while it deviates from older computations. Additionally, the analysis of line profiles suggests that, in some cases, the spectral resolution was insufficient to fully resolve dynamic substructures within the galaxies. Our results emphasize the importance of improved data quality and consistency for future studies, especially for future searches of finestructure constant variations at higher redshifts using this method.</p>
	]]></content:encoded>

	<dc:title>Line Ratio in the C-like Ion Spectrum O III: Testing Atomic Theory Predictions Through the Observation of Galaxies</dc:title>
			<dc:creator>Julius Richard Dreisbach</dc:creator>
			<dc:creator>Dominik J. Bomans</dc:creator>
			<dc:creator>Elmar Träbert</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4010003</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-02-10</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-02-10</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>3</prism:startingPage>
		<prism:doi>10.3390/astronomy4010003</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/1/2">

	<title>Astronomy, Vol. 4, Pages 2: Tracing the Evolution of the Emission Properties of Carbon-Rich AGB, Post-AGB, and PN Sources</title>
	<link>https://www.mdpi.com/2674-0346/4/1/2</link>
	<description>Understanding the transition from the Asymptotic Giant Branch (AGB) to the Planetary Nebula (PN) phase is crucial for advancing our knowledge of galaxy evolution and the chemical enrichment of the universe. In this manuscript, we analyze 137 carbon-rich, evolved low- and intermediate-mass stars (LIMSs) from both the Magellanic Clouds (MCs) and the Milky Way (MW). We focus on AGB, post-AGB, and PN sources, tracing the evolution of their emission through spectral energy distribution (SED) modeling. Consistent with previous studies, we observe that more evolved LIMSs exhibit cooler dust temperatures and lower optical depths. Amorphous carbon (amC) is the dominant dust species in all the evolutionary stages examined in this work, while silicon carbide (SiC) accounts for 5&amp;amp;ndash;30% of the total dust content. Additionally, we analyze color&amp;amp;ndash;color diagrams (CCDs) in the infrared using data from IRAC, WISE, and 2MASS, uncovering significant evolutionary trends in LIMS emission. AGB stars evolve from bluer to redder colors as they produce increasing amounts of dust. Post-AGB and PN sources are clearly differentiated from AGB stars, reflecting shifts in both effective stellar and dust temperatures as the stars transition through these evolutionary phases.</description>
	<pubDate>2025-01-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 2: Tracing the Evolution of the Emission Properties of Carbon-Rich AGB, Post-AGB, and PN Sources</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/1/2">doi: 10.3390/astronomy4010002</a></p>
	<p>Authors:
		Silvia Tosi
		Ester Marini
		</p>
	<p>Understanding the transition from the Asymptotic Giant Branch (AGB) to the Planetary Nebula (PN) phase is crucial for advancing our knowledge of galaxy evolution and the chemical enrichment of the universe. In this manuscript, we analyze 137 carbon-rich, evolved low- and intermediate-mass stars (LIMSs) from both the Magellanic Clouds (MCs) and the Milky Way (MW). We focus on AGB, post-AGB, and PN sources, tracing the evolution of their emission through spectral energy distribution (SED) modeling. Consistent with previous studies, we observe that more evolved LIMSs exhibit cooler dust temperatures and lower optical depths. Amorphous carbon (amC) is the dominant dust species in all the evolutionary stages examined in this work, while silicon carbide (SiC) accounts for 5&amp;amp;ndash;30% of the total dust content. Additionally, we analyze color&amp;amp;ndash;color diagrams (CCDs) in the infrared using data from IRAC, WISE, and 2MASS, uncovering significant evolutionary trends in LIMS emission. AGB stars evolve from bluer to redder colors as they produce increasing amounts of dust. Post-AGB and PN sources are clearly differentiated from AGB stars, reflecting shifts in both effective stellar and dust temperatures as the stars transition through these evolutionary phases.</p>
	]]></content:encoded>

	<dc:title>Tracing the Evolution of the Emission Properties of Carbon-Rich AGB, Post-AGB, and PN Sources</dc:title>
			<dc:creator>Silvia Tosi</dc:creator>
			<dc:creator>Ester Marini</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4010002</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-01-20</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-01-20</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/astronomy4010002</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/4/1/1">

	<title>Astronomy, Vol. 4, Pages 1: An Investigation of the Entropy Associated with a Collapsing Molecular Cloud</title>
	<link>https://www.mdpi.com/2674-0346/4/1/1</link>
	<description>The investigation of entropy variation during the star formation process within collapsing molecular clouds represents a significant field of inquiry in astrophysics. As the cloud contracts, the presence of gaseous components contributes to an increase in entropy; however, the degree of this entropy change is contingent upon the spatial constraints imposed on the gases. In this research endeavor, I perform a comprehensive analysis of entropy dynamics on a microcosmic level within the contracting cloud, adhering to the tenets of the second law of thermodynamics. The initial focus centers on a turbulent cloud consisting of N particles, each with a mass of M, which succumbs to gravitational forces. It becomes evident that for the collapse to transpire, the gravitational energy must surpass the opposing pressure forces, resulting in the swift movement of particles throughout the cloud and ultimately facilitating a shift in entropy.</description>
	<pubDate>2025-01-17</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 4, Pages 1: An Investigation of the Entropy Associated with a Collapsing Molecular Cloud</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/4/1/1">doi: 10.3390/astronomy4010001</a></p>
	<p>Authors:
		Gemechu Muleta Kumssa
		</p>
	<p>The investigation of entropy variation during the star formation process within collapsing molecular clouds represents a significant field of inquiry in astrophysics. As the cloud contracts, the presence of gaseous components contributes to an increase in entropy; however, the degree of this entropy change is contingent upon the spatial constraints imposed on the gases. In this research endeavor, I perform a comprehensive analysis of entropy dynamics on a microcosmic level within the contracting cloud, adhering to the tenets of the second law of thermodynamics. The initial focus centers on a turbulent cloud consisting of N particles, each with a mass of M, which succumbs to gravitational forces. It becomes evident that for the collapse to transpire, the gravitational energy must surpass the opposing pressure forces, resulting in the swift movement of particles throughout the cloud and ultimately facilitating a shift in entropy.</p>
	]]></content:encoded>

	<dc:title>An Investigation of the Entropy Associated with a Collapsing Molecular Cloud</dc:title>
			<dc:creator>Gemechu Muleta Kumssa</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy4010001</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2025-01-17</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2025-01-17</prism:publicationDate>
	<prism:volume>4</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/astronomy4010001</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/4/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/4/20">

	<title>Astronomy, Vol. 3, Pages 319-333: Axion Mass and the Ground State of Deconfining SU(2) Yang&amp;ndash;Mills Thermodynamics</title>
	<link>https://www.mdpi.com/2674-0346/3/4/20</link>
	<description>For the deconfinement phase of an SU(2) Yang&amp;amp;ndash;Mills theory, we compute the axion mass mA by appealing to the Veneziano&amp;amp;ndash;Witten formula. The topological susceptibility &amp;amp;chi; arises (i) from a precisely computable thermal ground-state contribution due to a center of a relevant (anti)caloron, and (ii) from contributions due to free thermal quasi-particles in the effective theory. Both (i) and (ii) are derived by using standard Euclidean thermal field theory techniques. While contribution (i) is positive and &amp;amp;prop;T4, contribution (ii) is negative, as demanded by reflection positivity, but negligible compared to contribution (i). As a consequence, practically from the critical temperature Tc onward, a real-valued axion mass mA(T)=23&amp;amp;pi;T2MP emerges when the Peccei&amp;amp;ndash;Quinn scale is assumed to be the Planck mass MP, independently of the Yang&amp;amp;ndash;Mills scale that the axion associates with. We discuss why our results deviate from those found in the dilute instanton gas and interacting instanton liquid approximations, and from results obtained in lattice simulations. Assuming the universe is dark sector to be based on such ultralight axion species, which are nonrelativistic for T&amp;amp;#8810;MP, we investigate the cosmological conditions for their global Bose condensation as the very early universe cooled to temperatures of the order of 109eV.</description>
	<pubDate>2024-12-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 319-333: Axion Mass and the Ground State of Deconfining SU(2) Yang&amp;ndash;Mills Thermodynamics</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/4/20">doi: 10.3390/astronomy3040020</a></p>
	<p>Authors:
		Ralf Hofmann
		Janning Meinert
		Dmitry Antonov
		</p>
	<p>For the deconfinement phase of an SU(2) Yang&amp;amp;ndash;Mills theory, we compute the axion mass mA by appealing to the Veneziano&amp;amp;ndash;Witten formula. The topological susceptibility &amp;amp;chi; arises (i) from a precisely computable thermal ground-state contribution due to a center of a relevant (anti)caloron, and (ii) from contributions due to free thermal quasi-particles in the effective theory. Both (i) and (ii) are derived by using standard Euclidean thermal field theory techniques. While contribution (i) is positive and &amp;amp;prop;T4, contribution (ii) is negative, as demanded by reflection positivity, but negligible compared to contribution (i). As a consequence, practically from the critical temperature Tc onward, a real-valued axion mass mA(T)=23&amp;amp;pi;T2MP emerges when the Peccei&amp;amp;ndash;Quinn scale is assumed to be the Planck mass MP, independently of the Yang&amp;amp;ndash;Mills scale that the axion associates with. We discuss why our results deviate from those found in the dilute instanton gas and interacting instanton liquid approximations, and from results obtained in lattice simulations. Assuming the universe is dark sector to be based on such ultralight axion species, which are nonrelativistic for T&amp;amp;#8810;MP, we investigate the cosmological conditions for their global Bose condensation as the very early universe cooled to temperatures of the order of 109eV.</p>
	]]></content:encoded>

	<dc:title>Axion Mass and the Ground State of Deconfining SU(2) Yang&amp;amp;ndash;Mills Thermodynamics</dc:title>
			<dc:creator>Ralf Hofmann</dc:creator>
			<dc:creator>Janning Meinert</dc:creator>
			<dc:creator>Dmitry Antonov</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3040020</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-12-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-12-18</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>319</prism:startingPage>
		<prism:doi>10.3390/astronomy3040020</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/4/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/4/19">

	<title>Astronomy, Vol. 3, Pages 304-318: Towards the Particle Spectrum, Tickled by a Distant Massive Object</title>
	<link>https://www.mdpi.com/2674-0346/3/4/19</link>
	<description>To investigate the gravitational effects of massive objects on a typical observer, we studied the dynamics of a test particle following BMS3 geodesics. We constructed the BMS3 framework using the canonical phase space formalism and the corresponding Hamiltonian. We focused on analyzing these effects at fine scales of spacetime, which led us to quantization of the phase space. By deriving and studying the solutions of the quantum equations of motion for the test particle, we obtained its energy spectrum and explored the behavior of its wave function. These findings offer a fresh perspective on gravitational interactions in the context of quantum mechanics, providing an alternative approach to traditional quantum field theory analyses.</description>
	<pubDate>2024-12-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 304-318: Towards the Particle Spectrum, Tickled by a Distant Massive Object</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/4/19">doi: 10.3390/astronomy3040019</a></p>
	<p>Authors:
		Mehdi Dehghani
		Salman A. Nejad
		Maryam Mardaani
		</p>
	<p>To investigate the gravitational effects of massive objects on a typical observer, we studied the dynamics of a test particle following BMS3 geodesics. We constructed the BMS3 framework using the canonical phase space formalism and the corresponding Hamiltonian. We focused on analyzing these effects at fine scales of spacetime, which led us to quantization of the phase space. By deriving and studying the solutions of the quantum equations of motion for the test particle, we obtained its energy spectrum and explored the behavior of its wave function. These findings offer a fresh perspective on gravitational interactions in the context of quantum mechanics, providing an alternative approach to traditional quantum field theory analyses.</p>
	]]></content:encoded>

	<dc:title>Towards the Particle Spectrum, Tickled by a Distant Massive Object</dc:title>
			<dc:creator>Mehdi Dehghani</dc:creator>
			<dc:creator>Salman A. Nejad</dc:creator>
			<dc:creator>Maryam Mardaani</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3040019</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-12-12</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-12-12</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>304</prism:startingPage>
		<prism:doi>10.3390/astronomy3040019</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/4/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/4/18">

	<title>Astronomy, Vol. 3, Pages 289-303: The Complex Structure of the Abell 548&amp;ndash;Abell 3367 Region</title>
	<link>https://www.mdpi.com/2674-0346/3/4/18</link>
	<description>Archival XMM and ROSAT X-Ray data are used to investigate the structure of the Abell 548&amp;amp;ndash;Abell 3367 region. Based on previous optical studies, this is a region likely to be rich in structure, although studies are in disagreement regarding the connection between Abell 3367 and Abell 548. We use the available archival X-Ray data together with kinematic data of counterpart galaxies to address this question and determine the structure in this region. The region is particularly rich in X-Ray structure elongated along a SW-NE axis and consisting of numerous extended X-Ray sources. In general, the structure consists of many galaxy groups and clusters which appear segregated in X-Ray luminosity, with the least luminous ~30% toward the outer region of the clusters, possibly tracing a filament. We find evidence to suggest a supercluster of three clusters at redshifts ~0.04, 0.045, and 0.06. Several of the X-Ray sources coincident with Abell 3367 have counterpart galaxy redshifts consistent with Abell 548, while others are significantly higher. This supports the formation of a supercluster consisting of Abell 548 and Abell 3667, with the higher-redshift X-Ray source being a background object. In addition, they are part of a larger structure consisting of a previously identified cluster at redshift 0.04 and two groups at redshift ~0.06. There is also filamentary structure at z ~0.103. The ubiquity of groups in the large-scale structure suggests that they provide an environment where galaxies are in close proximity and evolution via interaction can proceed well before the galaxies make their way into the dense central region of a cluster.</description>
	<pubDate>2024-11-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 289-303: The Complex Structure of the Abell 548&amp;ndash;Abell 3367 Region</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/4/18">doi: 10.3390/astronomy3040018</a></p>
	<p>Authors:
		Mark J. Henriksen
		Layla Ahmed
		</p>
	<p>Archival XMM and ROSAT X-Ray data are used to investigate the structure of the Abell 548&amp;amp;ndash;Abell 3367 region. Based on previous optical studies, this is a region likely to be rich in structure, although studies are in disagreement regarding the connection between Abell 3367 and Abell 548. We use the available archival X-Ray data together with kinematic data of counterpart galaxies to address this question and determine the structure in this region. The region is particularly rich in X-Ray structure elongated along a SW-NE axis and consisting of numerous extended X-Ray sources. In general, the structure consists of many galaxy groups and clusters which appear segregated in X-Ray luminosity, with the least luminous ~30% toward the outer region of the clusters, possibly tracing a filament. We find evidence to suggest a supercluster of three clusters at redshifts ~0.04, 0.045, and 0.06. Several of the X-Ray sources coincident with Abell 3367 have counterpart galaxy redshifts consistent with Abell 548, while others are significantly higher. This supports the formation of a supercluster consisting of Abell 548 and Abell 3667, with the higher-redshift X-Ray source being a background object. In addition, they are part of a larger structure consisting of a previously identified cluster at redshift 0.04 and two groups at redshift ~0.06. There is also filamentary structure at z ~0.103. The ubiquity of groups in the large-scale structure suggests that they provide an environment where galaxies are in close proximity and evolution via interaction can proceed well before the galaxies make their way into the dense central region of a cluster.</p>
	]]></content:encoded>

	<dc:title>The Complex Structure of the Abell 548&amp;amp;ndash;Abell 3367 Region</dc:title>
			<dc:creator>Mark J. Henriksen</dc:creator>
			<dc:creator>Layla Ahmed</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3040018</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-11-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-11-18</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>289</prism:startingPage>
		<prism:doi>10.3390/astronomy3040018</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/4/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/4/17">

	<title>Astronomy, Vol. 3, Pages 275-288: Separating the Spectral Counterparts in NGC 1275/Perseus Cluster in X-Rays</title>
	<link>https://www.mdpi.com/2674-0346/3/4/17</link>
	<description>We present a model-independent method for separating the spectral counterparts of the active galactic nucleus (AGN) NGC 1275 from the surrounding emission of the Perseus cluster, as observed by Suzaku/XIS cameras. The Perseus cluster emission extends to higher energies than typically observed in AGN environments, reaching up to 9&amp;amp;ndash;10 keV. This necessitates precise separation of AGN and cluster spectra. To circumvent the degeneracy arising from numerous spectral fitting parameters, including elemental abundances, thermal and Compton emissions from the nucleus, and spectral parameters of the jet synchrotron self-Compton/inverse Compton emissions, we avoid traditional spectral fitting methods. Instead, we leverage spatial resolution and employ a double background subtraction approach. We apply this procedure to the complete set of Suzaku/XIS observational data for NGC 1275, resulting in cleaned spectra and a light curve of the AGN emission in this system. To demonstrate the applicability of our method, we also utilize the available XMM-Newton/EPIC data.</description>
	<pubDate>2024-10-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 275-288: Separating the Spectral Counterparts in NGC 1275/Perseus Cluster in X-Rays</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/4/17">doi: 10.3390/astronomy3040017</a></p>
	<p>Authors:
		Elena Fedorova
		Lidiia Zadorozhna
		Anatolii Tugay
		Nadiia Pulatova
		Alexander Ganz
		Olexandr Gugnin
		</p>
	<p>We present a model-independent method for separating the spectral counterparts of the active galactic nucleus (AGN) NGC 1275 from the surrounding emission of the Perseus cluster, as observed by Suzaku/XIS cameras. The Perseus cluster emission extends to higher energies than typically observed in AGN environments, reaching up to 9&amp;amp;ndash;10 keV. This necessitates precise separation of AGN and cluster spectra. To circumvent the degeneracy arising from numerous spectral fitting parameters, including elemental abundances, thermal and Compton emissions from the nucleus, and spectral parameters of the jet synchrotron self-Compton/inverse Compton emissions, we avoid traditional spectral fitting methods. Instead, we leverage spatial resolution and employ a double background subtraction approach. We apply this procedure to the complete set of Suzaku/XIS observational data for NGC 1275, resulting in cleaned spectra and a light curve of the AGN emission in this system. To demonstrate the applicability of our method, we also utilize the available XMM-Newton/EPIC data.</p>
	]]></content:encoded>

	<dc:title>Separating the Spectral Counterparts in NGC 1275/Perseus Cluster in X-Rays</dc:title>
			<dc:creator>Elena Fedorova</dc:creator>
			<dc:creator>Lidiia Zadorozhna</dc:creator>
			<dc:creator>Anatolii Tugay</dc:creator>
			<dc:creator>Nadiia Pulatova</dc:creator>
			<dc:creator>Alexander Ganz</dc:creator>
			<dc:creator>Olexandr Gugnin</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3040017</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-10-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-10-18</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>275</prism:startingPage>
		<prism:doi>10.3390/astronomy3040017</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/4/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/16">

	<title>Astronomy, Vol. 3, Pages 255-274: An Event Horizon &amp;lsquo;Firewall&amp;rsquo; Undergoing Cosmological Expansion</title>
	<link>https://www.mdpi.com/2674-0346/3/3/16</link>
	<description>We embed an object with a singular horizon structure, reminiscent of (but fundamentally different from, except in a limiting case) a black hole event horizon, in an expanding, spherically symmetric, homogeneous, Universe that has a positive cosmological constant. Conformal representation is discussed. There is a temperature/pressure singularity and a corresponding scalar curvature singularity at the horizon. The expanding singular horizon ultimately bounds the entire spacetime manifold. It is is preceded by an expanding light front, which separates the spacetime affected by the singularity from that which is not yet affected. An appropriately located observer in front of the light front can have a Hubble&amp;amp;ndash;Lema&amp;amp;icirc;tre constant that is consistent with that currently observed.</description>
	<pubDate>2024-09-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 255-274: An Event Horizon &amp;lsquo;Firewall&amp;rsquo; Undergoing Cosmological Expansion</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/16">doi: 10.3390/astronomy3030016</a></p>
	<p>Authors:
		Richard N. Henriksen
		A. Gordon Emslie
		</p>
	<p>We embed an object with a singular horizon structure, reminiscent of (but fundamentally different from, except in a limiting case) a black hole event horizon, in an expanding, spherically symmetric, homogeneous, Universe that has a positive cosmological constant. Conformal representation is discussed. There is a temperature/pressure singularity and a corresponding scalar curvature singularity at the horizon. The expanding singular horizon ultimately bounds the entire spacetime manifold. It is is preceded by an expanding light front, which separates the spacetime affected by the singularity from that which is not yet affected. An appropriately located observer in front of the light front can have a Hubble&amp;amp;ndash;Lema&amp;amp;icirc;tre constant that is consistent with that currently observed.</p>
	]]></content:encoded>

	<dc:title>An Event Horizon &amp;amp;lsquo;Firewall&amp;amp;rsquo; Undergoing Cosmological Expansion</dc:title>
			<dc:creator>Richard N. Henriksen</dc:creator>
			<dc:creator>A. Gordon Emslie</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030016</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-09-23</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-09-23</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>255</prism:startingPage>
		<prism:doi>10.3390/astronomy3030016</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/15">

	<title>Astronomy, Vol. 3, Pages 240-254: Antineutrino Opacity in Neutron Stars in Models Constrained by Recent Terrestrial Experiments and Astrophysical Observations</title>
	<link>https://www.mdpi.com/2674-0346/3/3/15</link>
	<description>Inthe present paper, we investigate neutral current (NC) antineutrino scattering with the constituents of neutron star (NS) matter at zero temperature. The modeling of standard matter in NS is constructed within the framework of both extended relativistic mean-field (E-RMF) and nonrelativistic Korea-IBS-Daegu-SKKU energy density functional (KIDS-EDF) models. In the E-RMF model, we use a new parameter, G3(M), which was constrained by the recent PREX II experiment measurement of neutron distribution in 208Pb, while the KIDS-EDF models are constrained by terrestrial experiments, gravitational-wave signals, and astrophysical observations. Using both realistic and well-constrained matter models, we then calculate the antineutrino differential cross-section (ADCS) and antineutrino mean free path (AMFP) for the interaction between antineutrinos and neutron star (NS) matter constituents using linear response theory. It is found that the AMFP for the KIDS0 and KIDSA models are smaller compared to the SLy4 model and the E-RMF model with the G3(M) parameter. The AMFP result of the Skyrme model with the SLy4 parameter set is found to have a prediction almost similar to that of the E-RMF model with the G3(M) parameter. Contributions of each nucleon to the total AMFP are also presented for the G3(M) model.</description>
	<pubDate>2024-08-27</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 240-254: Antineutrino Opacity in Neutron Stars in Models Constrained by Recent Terrestrial Experiments and Astrophysical Observations</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/15">doi: 10.3390/astronomy3030015</a></p>
	<p>Authors:
		Parada T. P. Hutauruk
		</p>
	<p>Inthe present paper, we investigate neutral current (NC) antineutrino scattering with the constituents of neutron star (NS) matter at zero temperature. The modeling of standard matter in NS is constructed within the framework of both extended relativistic mean-field (E-RMF) and nonrelativistic Korea-IBS-Daegu-SKKU energy density functional (KIDS-EDF) models. In the E-RMF model, we use a new parameter, G3(M), which was constrained by the recent PREX II experiment measurement of neutron distribution in 208Pb, while the KIDS-EDF models are constrained by terrestrial experiments, gravitational-wave signals, and astrophysical observations. Using both realistic and well-constrained matter models, we then calculate the antineutrino differential cross-section (ADCS) and antineutrino mean free path (AMFP) for the interaction between antineutrinos and neutron star (NS) matter constituents using linear response theory. It is found that the AMFP for the KIDS0 and KIDSA models are smaller compared to the SLy4 model and the E-RMF model with the G3(M) parameter. The AMFP result of the Skyrme model with the SLy4 parameter set is found to have a prediction almost similar to that of the E-RMF model with the G3(M) parameter. Contributions of each nucleon to the total AMFP are also presented for the G3(M) model.</p>
	]]></content:encoded>

	<dc:title>Antineutrino Opacity in Neutron Stars in Models Constrained by Recent Terrestrial Experiments and Astrophysical Observations</dc:title>
			<dc:creator>Parada T. P. Hutauruk</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030015</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-08-27</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-08-27</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>240</prism:startingPage>
		<prism:doi>10.3390/astronomy3030015</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/14">

	<title>Astronomy, Vol. 3, Pages 220-239: Shell Universe: Reducing Cosmological Tensions with the Relativistic Ni Solutions</title>
	<link>https://www.mdpi.com/2674-0346/3/3/14</link>
	<description>Recent discoveries of massive galaxies existing in the early universe, as well as apparent anomalies in &amp;amp;Omega;m and H0 at high redshift, have raised sharp new concerns for the &amp;amp;Lambda;CDM model of cosmology. Here, we address these problems by using new solutions for the Einstein field equations of relativistic compact objects originally found by Ni. Applied to the universe, the new solutions imply that the universe&amp;amp;rsquo;s mass is relatively concentrated in a thick outer shell. The interior space would not have a flat, Minkowski metric, but rather a repulsive gravitational field centered on the origin. This field would induce a gravitational redshift in light waves moving inward from the cosmic shell and a corresponding blueshift in waves approaching the shell. Assuming the Milky Way lies near the origin, within the KBC Void, this redshift would make H0 appear to diminish at high redshifts and could thus relieve the Hubble tension. The Ni redshift could also reduce or eliminate the requirement for dark energy in the &amp;amp;Lambda;CDM model. The relative dimness of distant objects would instead arise because the Ni redshift makes them appear closer to us than they really are. To account for the CMB temperature&amp;amp;ndash;redshift relation and for the absence of a systematic blueshift in stars closer to the origin than the Milky Way, it is proposed that the Ni redshift and blueshift involve exchanges of photon energy with a photonic spacetime. These exchanges in turn form the basis for a cosmic CMB cycle, which gives rise to gravity and an Einsteinian cosmological constant, &amp;amp;Lambda;. Black holes are suggested to have analogous Ni structures and gravity/&amp;amp;Lambda; cycles.</description>
	<pubDate>2024-08-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 220-239: Shell Universe: Reducing Cosmological Tensions with the Relativistic Ni Solutions</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/14">doi: 10.3390/astronomy3030014</a></p>
	<p>Authors:
		Matthew R. Edwards
		</p>
	<p>Recent discoveries of massive galaxies existing in the early universe, as well as apparent anomalies in &amp;amp;Omega;m and H0 at high redshift, have raised sharp new concerns for the &amp;amp;Lambda;CDM model of cosmology. Here, we address these problems by using new solutions for the Einstein field equations of relativistic compact objects originally found by Ni. Applied to the universe, the new solutions imply that the universe&amp;amp;rsquo;s mass is relatively concentrated in a thick outer shell. The interior space would not have a flat, Minkowski metric, but rather a repulsive gravitational field centered on the origin. This field would induce a gravitational redshift in light waves moving inward from the cosmic shell and a corresponding blueshift in waves approaching the shell. Assuming the Milky Way lies near the origin, within the KBC Void, this redshift would make H0 appear to diminish at high redshifts and could thus relieve the Hubble tension. The Ni redshift could also reduce or eliminate the requirement for dark energy in the &amp;amp;Lambda;CDM model. The relative dimness of distant objects would instead arise because the Ni redshift makes them appear closer to us than they really are. To account for the CMB temperature&amp;amp;ndash;redshift relation and for the absence of a systematic blueshift in stars closer to the origin than the Milky Way, it is proposed that the Ni redshift and blueshift involve exchanges of photon energy with a photonic spacetime. These exchanges in turn form the basis for a cosmic CMB cycle, which gives rise to gravity and an Einsteinian cosmological constant, &amp;amp;Lambda;. Black holes are suggested to have analogous Ni structures and gravity/&amp;amp;Lambda; cycles.</p>
	]]></content:encoded>

	<dc:title>Shell Universe: Reducing Cosmological Tensions with the Relativistic Ni Solutions</dc:title>
			<dc:creator>Matthew R. Edwards</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030014</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-08-07</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-08-07</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>220</prism:startingPage>
		<prism:doi>10.3390/astronomy3030014</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/13">

	<title>Astronomy, Vol. 3, Pages 208-219: Periods of Outbursts and Standstills and Variations in Parameters of Two Z Cam Stars: Z Cam and AT Cnc</title>
	<link>https://www.mdpi.com/2674-0346/3/3/13</link>
	<description>We present our results on two Z Cam stars: Z Cam and AT Cnc. We apply observational data for the periods that cover the states of outbursts and standstills, which are typical for this type of object. We report an appearance of periodic oscillations in brightness during the standstill in AT Cnc, with small-amplitude variations of 0.03&amp;amp;ndash;0.04 mag and periodicity of &amp;amp;asymp;20&amp;amp;ndash;30 min. Based on the estimated dereddened color index (B &amp;amp;minus; V)0, we calculate the color temperature for both states of the two objects. During the transition from the outburst to the standstill state, Z Cam varies from bluer to redder, while AT Cnc stays redder in both states. We calculate some of the stars&amp;amp;rsquo; parameters as the radii of the primary and secondary components and the orbital separation for both objects. We construct the profiles of the effective temperature in the discs of the two objects. Comparing the parameters of both systems, we see that Z Cam is definitely the hotter object and we conclude that it has a more active accretion disc.</description>
	<pubDate>2024-08-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 208-219: Periods of Outbursts and Standstills and Variations in Parameters of Two Z Cam Stars: Z Cam and AT Cnc</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/13">doi: 10.3390/astronomy3030013</a></p>
	<p>Authors:
		Daniela Boneva
		Krasimira Yankova
		Denislav Rusev
		</p>
	<p>We present our results on two Z Cam stars: Z Cam and AT Cnc. We apply observational data for the periods that cover the states of outbursts and standstills, which are typical for this type of object. We report an appearance of periodic oscillations in brightness during the standstill in AT Cnc, with small-amplitude variations of 0.03&amp;amp;ndash;0.04 mag and periodicity of &amp;amp;asymp;20&amp;amp;ndash;30 min. Based on the estimated dereddened color index (B &amp;amp;minus; V)0, we calculate the color temperature for both states of the two objects. During the transition from the outburst to the standstill state, Z Cam varies from bluer to redder, while AT Cnc stays redder in both states. We calculate some of the stars&amp;amp;rsquo; parameters as the radii of the primary and secondary components and the orbital separation for both objects. We construct the profiles of the effective temperature in the discs of the two objects. Comparing the parameters of both systems, we see that Z Cam is definitely the hotter object and we conclude that it has a more active accretion disc.</p>
	]]></content:encoded>

	<dc:title>Periods of Outbursts and Standstills and Variations in Parameters of Two Z Cam Stars: Z Cam and AT Cnc</dc:title>
			<dc:creator>Daniela Boneva</dc:creator>
			<dc:creator>Krasimira Yankova</dc:creator>
			<dc:creator>Denislav Rusev</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030013</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-08-01</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-08-01</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>208</prism:startingPage>
		<prism:doi>10.3390/astronomy3030013</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/12">

	<title>Astronomy, Vol. 3, Pages 189-207: Unsupervised Domain Adaptation for Constraining Star Formation Histories</title>
	<link>https://www.mdpi.com/2674-0346/3/3/12</link>
	<description>In astronomy, understanding the evolutionary trajectories of galaxies necessitates a robust analysis of their star formation histories (SFHs), a task complicated by our inability to observe these vast celestial entities throughout their billion-year lifespans. This study pioneers the application of the Kullback&amp;amp;ndash;Leibler Importance Estimation Procedure (KLIEP), an unsupervised domain adaptation technique, to address this challenge. By adeptly applying KLIEP, we harness the power of machine learning to innovatively predict SFHs, utilizing simulated galaxy models to forge a novel linkage between simulation and observation. This methodology signifies a substantial advancement beyond the traditional Bayesian approaches to Spectral Energy Distribution (SED) analysis, which are often undermined by the absence of empirical SFH benchmarks. Our empirical investigations reveal that KLIEP markedly enhances the precision and reliability of SFH inference, offering a significant leap forward compared to existing methodologies. The results underscore the potential of KLIEP in refining our comprehension of galactic evolution, paving the way for its application in analyzing actual astronomical observations. Accompanying this paper, we provide access to the supporting code and dataset on GitHub, encouraging further exploration and validation of the efficacy of the KLIEP in the field.</description>
	<pubDate>2024-07-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 189-207: Unsupervised Domain Adaptation for Constraining Star Formation Histories</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/12">doi: 10.3390/astronomy3030012</a></p>
	<p>Authors:
		Sankalp Gilda
		Antoine de Mathelin
		Sabine Bellstedt
		Guillaume Richard
		</p>
	<p>In astronomy, understanding the evolutionary trajectories of galaxies necessitates a robust analysis of their star formation histories (SFHs), a task complicated by our inability to observe these vast celestial entities throughout their billion-year lifespans. This study pioneers the application of the Kullback&amp;amp;ndash;Leibler Importance Estimation Procedure (KLIEP), an unsupervised domain adaptation technique, to address this challenge. By adeptly applying KLIEP, we harness the power of machine learning to innovatively predict SFHs, utilizing simulated galaxy models to forge a novel linkage between simulation and observation. This methodology signifies a substantial advancement beyond the traditional Bayesian approaches to Spectral Energy Distribution (SED) analysis, which are often undermined by the absence of empirical SFH benchmarks. Our empirical investigations reveal that KLIEP markedly enhances the precision and reliability of SFH inference, offering a significant leap forward compared to existing methodologies. The results underscore the potential of KLIEP in refining our comprehension of galactic evolution, paving the way for its application in analyzing actual astronomical observations. Accompanying this paper, we provide access to the supporting code and dataset on GitHub, encouraging further exploration and validation of the efficacy of the KLIEP in the field.</p>
	]]></content:encoded>

	<dc:title>Unsupervised Domain Adaptation for Constraining Star Formation Histories</dc:title>
			<dc:creator>Sankalp Gilda</dc:creator>
			<dc:creator>Antoine de Mathelin</dc:creator>
			<dc:creator>Sabine Bellstedt</dc:creator>
			<dc:creator>Guillaume Richard</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030012</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-07-03</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-07-03</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Conference Report</prism:section>
	<prism:startingPage>189</prism:startingPage>
		<prism:doi>10.3390/astronomy3030012</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/3/11">

	<title>Astronomy, Vol. 3, Pages 167-188: RisingTides: An Analytic Modeling Code of Tidal Effects in Binary Neutron Star Mergers</title>
	<link>https://www.mdpi.com/2674-0346/3/3/11</link>
	<description>Gravitational waves produced by binary neutron star mergers offer a unique window into matter behavior under extreme conditions. In this context, we analytically model the effect of matter on gravitational waves from binary neutron star mergers. We start with a binary black hole system, leveraging the post-Newtonian formalism for the inspiral and the Backwards-one-Body model for the merger. We combine the two methods to generate a baseline waveform and we validate our results against numerical relativity simulations. Next, we integrate tidal effects in phase and amplitude to account for matter and spacetime interaction using the NRTidal model and test its accuracy against numerical relativity predictions for two equations of state, finding a mismatch around the merger. Subsequently, we lift the restriction on the coefficients to be independent of the tidal deformability and recalibrate them using the numerical relativity predictions. We obtain better fits for phase and amplitude around the merger and are able to extend the phase modeling beyond the merger. We implement our method in new open-source, user-friendly Python code, steered by a Jupyter Notebook, named RisingTides. Our research offers new perspectives on analytically modeling the effect of tides on the gravitational waves from binary neutron star mergers.</description>
	<pubDate>2024-07-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 167-188: RisingTides: An Analytic Modeling Code of Tidal Effects in Binary Neutron Star Mergers</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/3/11">doi: 10.3390/astronomy3030011</a></p>
	<p>Authors:
		Alexander O’Dell
		Maria C. Babiuc Hamilton
		</p>
	<p>Gravitational waves produced by binary neutron star mergers offer a unique window into matter behavior under extreme conditions. In this context, we analytically model the effect of matter on gravitational waves from binary neutron star mergers. We start with a binary black hole system, leveraging the post-Newtonian formalism for the inspiral and the Backwards-one-Body model for the merger. We combine the two methods to generate a baseline waveform and we validate our results against numerical relativity simulations. Next, we integrate tidal effects in phase and amplitude to account for matter and spacetime interaction using the NRTidal model and test its accuracy against numerical relativity predictions for two equations of state, finding a mismatch around the merger. Subsequently, we lift the restriction on the coefficients to be independent of the tidal deformability and recalibrate them using the numerical relativity predictions. We obtain better fits for phase and amplitude around the merger and are able to extend the phase modeling beyond the merger. We implement our method in new open-source, user-friendly Python code, steered by a Jupyter Notebook, named RisingTides. Our research offers new perspectives on analytically modeling the effect of tides on the gravitational waves from binary neutron star mergers.</p>
	]]></content:encoded>

	<dc:title>RisingTides: An Analytic Modeling Code of Tidal Effects in Binary Neutron Star Mergers</dc:title>
			<dc:creator>Alexander O’Dell</dc:creator>
			<dc:creator>Maria C. Babiuc Hamilton</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3030011</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-07-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-07-02</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>167</prism:startingPage>
		<prism:doi>10.3390/astronomy3030011</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/3/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/2/10">

	<title>Astronomy, Vol. 3, Pages 139-166: Landau Tidal Damping and Major-Body Clustering in Solar and Extrasolar Subsystems</title>
	<link>https://www.mdpi.com/2674-0346/3/2/10</link>
	<description>Major (exo)planetary and satellite bodies seem to concentrate at intermediate areas of the radial distributions of all the objects orbiting in each (sub)system. We show that angular-momentum transport during secular evolution of (exo)planets and satellites necessarily results in the observed intermediate accumulation of the massive objects. We quantify the &amp;amp;lsquo;middle&amp;amp;rsquo; as the mean of mean motions (orbital angular velocities) when three or more massive objects are involved. Radial evolution of the orbits is expected to be halted when the survivors settle near mean-motion resonances and angular-momentum transfer between them ceases (gravitational Landau damping). This dynamical behavior is opposite in direction to what has been theorized for viscous and magnetized accretion disks, in which gas spreads out and away from either side of any conceivable intermediate area. We present angular momentum transfer calculations in few-body systems, and we also calculate the tidal dissipation timescales and the physical properties of the mean tidal field in planetary and satellite (sub)systems.</description>
	<pubDate>2024-06-04</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 139-166: Landau Tidal Damping and Major-Body Clustering in Solar and Extrasolar Subsystems</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/2/10">doi: 10.3390/astronomy3020010</a></p>
	<p>Authors:
		Dimitris M. Christodoulou
		Demosthenes Kazanas
		</p>
	<p>Major (exo)planetary and satellite bodies seem to concentrate at intermediate areas of the radial distributions of all the objects orbiting in each (sub)system. We show that angular-momentum transport during secular evolution of (exo)planets and satellites necessarily results in the observed intermediate accumulation of the massive objects. We quantify the &amp;amp;lsquo;middle&amp;amp;rsquo; as the mean of mean motions (orbital angular velocities) when three or more massive objects are involved. Radial evolution of the orbits is expected to be halted when the survivors settle near mean-motion resonances and angular-momentum transfer between them ceases (gravitational Landau damping). This dynamical behavior is opposite in direction to what has been theorized for viscous and magnetized accretion disks, in which gas spreads out and away from either side of any conceivable intermediate area. We present angular momentum transfer calculations in few-body systems, and we also calculate the tidal dissipation timescales and the physical properties of the mean tidal field in planetary and satellite (sub)systems.</p>
	]]></content:encoded>

	<dc:title>Landau Tidal Damping and Major-Body Clustering in Solar and Extrasolar Subsystems</dc:title>
			<dc:creator>Dimitris M. Christodoulou</dc:creator>
			<dc:creator>Demosthenes Kazanas</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3020010</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-06-04</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-06-04</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>139</prism:startingPage>
		<prism:doi>10.3390/astronomy3020010</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/2/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/2/9">

	<title>Astronomy, Vol. 3, Pages 122-138: Deep Sky Objects Detection with Deep Learning for Electronically Assisted Astronomy</title>
	<link>https://www.mdpi.com/2674-0346/3/2/9</link>
	<description>Electronically Assisted Astronomy is a fascinating activity requiring suitable conditions and expertise to be fully appreciated. Complex equipment, light pollution around urban areas and lack of contextual information often prevents newcomers from making the most of their observations, restricting the field to a niche expert audience. With recent smart telescopes, amateur and professional astronomers can capture efficiently a large number of images. However, post-hoc verification is still necessary to check whether deep sky objects are visible in the produced images, depending on their magnitude and observation conditions. If this detection can be performed during data acquisition, it would be possible to configure the capture time more precisely. While state-of-the-art works are focused on detection techniques for large surveys produced by professional ground-based observatories, we propose in this paper several Deep Learning approaches to detect celestial targets in images captured with smart telescopes, with a F1-score between 0.4 and 0.62 on test data, and we experimented them during outreach sessions with public in Luxembourg Greater Region.</description>
	<pubDate>2024-05-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 122-138: Deep Sky Objects Detection with Deep Learning for Electronically Assisted Astronomy</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/2/9">doi: 10.3390/astronomy3020009</a></p>
	<p>Authors:
		Olivier Parisot
		Mahmoud Jaziri
		</p>
	<p>Electronically Assisted Astronomy is a fascinating activity requiring suitable conditions and expertise to be fully appreciated. Complex equipment, light pollution around urban areas and lack of contextual information often prevents newcomers from making the most of their observations, restricting the field to a niche expert audience. With recent smart telescopes, amateur and professional astronomers can capture efficiently a large number of images. However, post-hoc verification is still necessary to check whether deep sky objects are visible in the produced images, depending on their magnitude and observation conditions. If this detection can be performed during data acquisition, it would be possible to configure the capture time more precisely. While state-of-the-art works are focused on detection techniques for large surveys produced by professional ground-based observatories, we propose in this paper several Deep Learning approaches to detect celestial targets in images captured with smart telescopes, with a F1-score between 0.4 and 0.62 on test data, and we experimented them during outreach sessions with public in Luxembourg Greater Region.</p>
	]]></content:encoded>

	<dc:title>Deep Sky Objects Detection with Deep Learning for Electronically Assisted Astronomy</dc:title>
			<dc:creator>Olivier Parisot</dc:creator>
			<dc:creator>Mahmoud Jaziri</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3020009</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-05-13</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-05-13</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>122</prism:startingPage>
		<prism:doi>10.3390/astronomy3020009</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/2/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/2/8">

	<title>Astronomy, Vol. 3, Pages 114-121: Constraining the Inner Galactic DM Density Profile with H.E.S.S.</title>
	<link>https://www.mdpi.com/2674-0346/3/2/8</link>
	<description>In this short review, corresponding to a talk given at the conference &amp;amp;ldquo;Cosmology 2023 in Miramare&amp;amp;rdquo;, we combine an analysis of five regions observed by H.E.S.S. in the Galactic Center, intending to constrain the Dark Matter (DM) density profile in a WIMP annihilation scenario. For the analysis, we include the state-of-the-art Galactic diffuse emission Gamma-optimized model computed with DRAGON and a wide range of DM density profiles from cored to cuspy profiles, including different kinds of DM spikes. Our results are able to constrain generalized NFW profiles with an inner slope &amp;amp;gamma;&amp;amp;#8819;1.3. When considering DM spikes, the adiabatic spike is completely ruled out. However, smoother spikes given by the interactions with the bulge stars are compatible if &amp;amp;gamma;&amp;amp;#8818;0.8, with an internal slope of &amp;amp;gamma;sp-stars=1.5.</description>
	<pubDate>2024-04-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 114-121: Constraining the Inner Galactic DM Density Profile with H.E.S.S.</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/2/8">doi: 10.3390/astronomy3020008</a></p>
	<p>Authors:
		Jaume Zuriaga-Puig
		</p>
	<p>In this short review, corresponding to a talk given at the conference &amp;amp;ldquo;Cosmology 2023 in Miramare&amp;amp;rdquo;, we combine an analysis of five regions observed by H.E.S.S. in the Galactic Center, intending to constrain the Dark Matter (DM) density profile in a WIMP annihilation scenario. For the analysis, we include the state-of-the-art Galactic diffuse emission Gamma-optimized model computed with DRAGON and a wide range of DM density profiles from cored to cuspy profiles, including different kinds of DM spikes. Our results are able to constrain generalized NFW profiles with an inner slope &amp;amp;gamma;&amp;amp;#8819;1.3. When considering DM spikes, the adiabatic spike is completely ruled out. However, smoother spikes given by the interactions with the bulge stars are compatible if &amp;amp;gamma;&amp;amp;#8818;0.8, with an internal slope of &amp;amp;gamma;sp-stars=1.5.</p>
	]]></content:encoded>

	<dc:title>Constraining the Inner Galactic DM Density Profile with H.E.S.S.</dc:title>
			<dc:creator>Jaume Zuriaga-Puig</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3020008</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-04-11</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-04-11</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Brief Report</prism:section>
	<prism:startingPage>114</prism:startingPage>
		<prism:doi>10.3390/astronomy3020008</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/2/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/2/7">

	<title>Astronomy, Vol. 3, Pages 100-113: Cosmography of the Minimally Extended Varying Speed-of-Light Model</title>
	<link>https://www.mdpi.com/2674-0346/3/2/7</link>
	<description>Cosmography, as an integral branch of cosmology, strives to characterize the Universe without relying on pre-determined cosmological models. This model-independent approach utilizes Taylor series expansions around the current epoch, providing a direct correlation with cosmological observations and the potential to constrain theoretical models. Various observable quantities in cosmology can be described as different combinations of cosmographic parameters. Furthermore, one can apply cosmography to models with a varying speed of light. In this case, the Hubble parameter can be expressed by the same combination of cosmographic parameters for both the standard model and varying speed-of-light models. However, for the luminosity distance, the two models are represented by different combinations of cosmographic parameters. Hence, luminosity distance might provide a method to constrain the parameters in varying speed-of-light models.</description>
	<pubDate>2024-04-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 100-113: Cosmography of the Minimally Extended Varying Speed-of-Light Model</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/2/7">doi: 10.3390/astronomy3020007</a></p>
	<p>Authors:
		Seokcheon Lee
		</p>
	<p>Cosmography, as an integral branch of cosmology, strives to characterize the Universe without relying on pre-determined cosmological models. This model-independent approach utilizes Taylor series expansions around the current epoch, providing a direct correlation with cosmological observations and the potential to constrain theoretical models. Various observable quantities in cosmology can be described as different combinations of cosmographic parameters. Furthermore, one can apply cosmography to models with a varying speed of light. In this case, the Hubble parameter can be expressed by the same combination of cosmographic parameters for both the standard model and varying speed-of-light models. However, for the luminosity distance, the two models are represented by different combinations of cosmographic parameters. Hence, luminosity distance might provide a method to constrain the parameters in varying speed-of-light models.</p>
	]]></content:encoded>

	<dc:title>Cosmography of the Minimally Extended Varying Speed-of-Light Model</dc:title>
			<dc:creator>Seokcheon Lee</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3020007</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-04-07</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-04-07</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>100</prism:startingPage>
		<prism:doi>10.3390/astronomy3020007</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/2/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/2/6">

	<title>Astronomy, Vol. 3, Pages 68-99: Refracted Gravity Solutions from Small to Large Scales</title>
	<link>https://www.mdpi.com/2674-0346/3/2/6</link>
	<description>If visible matter alone is present in the Universe, general relativity (GR) and its Newtonian weak field limit (WFL) cannot explain several pieces of evidence, from the largest to the smallest scales. The most investigated solution is the cosmological model &amp;amp;Lambda; cold dark matter (&amp;amp;Lambda;CDM), where GR is valid and two dark components are introduced, dark energy (DE) and dark matter (DM), to explain the &amp;amp;sim;70% and &amp;amp;sim;25% of the mass&amp;amp;ndash;energy budget of the Universe, respectively. An alternative approach is provided by modified gravity theories, where a departure of the gravity law from &amp;amp;Lambda;CDM is assumed, and no dark components are included. This work presents refracted gravity (RG), a modified theory of gravity formulated in a classical way where the presence of DM is mimicked by a gravitational permittivity &amp;amp;#1013;(&amp;amp;rho;) monotonically increasing with the local mass density &amp;amp;rho;, which causes the field lines to be refracted in small density environments. Specifically, the flatter the system the stronger the refraction effect and thus, the larger the mass discrepancy if interpreted in Newtonian gravity. RG presented several encouraging results in modelling the dynamics of disk and elliptical galaxies and the temperature profiles of the hot X-ray emitting gas in galaxy clusters and a covariant extension of the theory seems to be promising.</description>
	<pubDate>2024-04-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 68-99: Refracted Gravity Solutions from Small to Large Scales</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/2/6">doi: 10.3390/astronomy3020006</a></p>
	<p>Authors:
		Valentina Cesare
		</p>
	<p>If visible matter alone is present in the Universe, general relativity (GR) and its Newtonian weak field limit (WFL) cannot explain several pieces of evidence, from the largest to the smallest scales. The most investigated solution is the cosmological model &amp;amp;Lambda; cold dark matter (&amp;amp;Lambda;CDM), where GR is valid and two dark components are introduced, dark energy (DE) and dark matter (DM), to explain the &amp;amp;sim;70% and &amp;amp;sim;25% of the mass&amp;amp;ndash;energy budget of the Universe, respectively. An alternative approach is provided by modified gravity theories, where a departure of the gravity law from &amp;amp;Lambda;CDM is assumed, and no dark components are included. This work presents refracted gravity (RG), a modified theory of gravity formulated in a classical way where the presence of DM is mimicked by a gravitational permittivity &amp;amp;#1013;(&amp;amp;rho;) monotonically increasing with the local mass density &amp;amp;rho;, which causes the field lines to be refracted in small density environments. Specifically, the flatter the system the stronger the refraction effect and thus, the larger the mass discrepancy if interpreted in Newtonian gravity. RG presented several encouraging results in modelling the dynamics of disk and elliptical galaxies and the temperature profiles of the hot X-ray emitting gas in galaxy clusters and a covariant extension of the theory seems to be promising.</p>
	]]></content:encoded>

	<dc:title>Refracted Gravity Solutions from Small to Large Scales</dc:title>
			<dc:creator>Valentina Cesare</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3020006</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-04-05</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-04-05</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>68</prism:startingPage>
		<prism:doi>10.3390/astronomy3020006</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/2/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/1/5">

	<title>Astronomy, Vol. 3, Pages 43-67: A Critical Examination of the Standard Cosmological Model: Toward a Modified Framework for Explaining Cosmic Structure Formation and Evolution</title>
	<link>https://www.mdpi.com/2674-0346/3/1/5</link>
	<description>This paper explores the fundamental cosmological principle, with a specific focus on the homogeneity and isotropy assumptions inherent in the Friedmann model that underpins the standard model. We propose a modified redshift model that is based on the spatial distribution of luminous matter, examining three key astronomical quantities: light intensity, number density, and the redshift of galaxies. Our analysis suggests that the model can account for cosmic accelerated expansion without the need for dark energy in the equations. Both simulations and analytical solutions reveal a unique pattern in the formation and evolution of cosmic structures, particularly in galaxy formation. This pattern shows a significant burst of activity between redshifts 0 &amp;amp;lt; z &amp;amp;lt; 0.4, which then progresses rapidly until approximately z &amp;amp;asymp; 0.9, indicating that the majority of cosmic structures were formed during this period. Subsequently, the process slows down considerably, reaching a nearly constant rate until around z &amp;amp;asymp; 1.6, after which a gradual decline begins. We also observe a distinctive redshift transition around z &amp;amp;asymp; 0.9 before the onset of dark-matter-induced accelerated expansion. This transition is directly related to the matter density and is dependent on the geometry of the universe. The model&amp;amp;rsquo;s ability to explain cosmic acceleration without requiring fine tuning of the cosmological constant highlights its novelty, providing a fresh perspective on the dynamic evolution of the universe.</description>
	<pubDate>2024-03-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 43-67: A Critical Examination of the Standard Cosmological Model: Toward a Modified Framework for Explaining Cosmic Structure Formation and Evolution</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/1/5">doi: 10.3390/astronomy3010005</a></p>
	<p>Authors:
		Robert Nyakundi Nyagisera
		Dismas Wamalwa
		Bernard Rapando
		Celline Awino
		Maxwell Mageto
		</p>
	<p>This paper explores the fundamental cosmological principle, with a specific focus on the homogeneity and isotropy assumptions inherent in the Friedmann model that underpins the standard model. We propose a modified redshift model that is based on the spatial distribution of luminous matter, examining three key astronomical quantities: light intensity, number density, and the redshift of galaxies. Our analysis suggests that the model can account for cosmic accelerated expansion without the need for dark energy in the equations. Both simulations and analytical solutions reveal a unique pattern in the formation and evolution of cosmic structures, particularly in galaxy formation. This pattern shows a significant burst of activity between redshifts 0 &amp;amp;lt; z &amp;amp;lt; 0.4, which then progresses rapidly until approximately z &amp;amp;asymp; 0.9, indicating that the majority of cosmic structures were formed during this period. Subsequently, the process slows down considerably, reaching a nearly constant rate until around z &amp;amp;asymp; 1.6, after which a gradual decline begins. We also observe a distinctive redshift transition around z &amp;amp;asymp; 0.9 before the onset of dark-matter-induced accelerated expansion. This transition is directly related to the matter density and is dependent on the geometry of the universe. The model&amp;amp;rsquo;s ability to explain cosmic acceleration without requiring fine tuning of the cosmological constant highlights its novelty, providing a fresh perspective on the dynamic evolution of the universe.</p>
	]]></content:encoded>

	<dc:title>A Critical Examination of the Standard Cosmological Model: Toward a Modified Framework for Explaining Cosmic Structure Formation and Evolution</dc:title>
			<dc:creator>Robert Nyakundi Nyagisera</dc:creator>
			<dc:creator>Dismas Wamalwa</dc:creator>
			<dc:creator>Bernard Rapando</dc:creator>
			<dc:creator>Celline Awino</dc:creator>
			<dc:creator>Maxwell Mageto</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3010005</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-03-12</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-03-12</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>43</prism:startingPage>
		<prism:doi>10.3390/astronomy3010005</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/1/4">

	<title>Astronomy, Vol. 3, Pages 29-42: Gravity on a Large Scale&amp;mdash;Does It Necessarily Look like It Does on a Small Scale?</title>
	<link>https://www.mdpi.com/2674-0346/3/1/4</link>
	<description>The notion of a local inertial reference frame is thoroughly analyzed. Dynamics of a field of such frames is derived from the variational principle. It is shown that the resulting theory splits naturally into three sectors, one of which is purely gravitational. Field dynamics in this sector, equivalent to Einstein&amp;amp;rsquo;s vacuum equations, is obtained unambiguously and admits no ad hoc corrections. The cosmological constant is an essential element of this construction and cannot be removed. It has been shown that the second sector of this theory corresponds to electrodynamics, while the last sector could possibly describe dark matter.</description>
	<pubDate>2024-03-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 29-42: Gravity on a Large Scale&amp;mdash;Does It Necessarily Look like It Does on a Small Scale?</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/1/4">doi: 10.3390/astronomy3010004</a></p>
	<p>Authors:
		Jerzy Kijowski
		</p>
	<p>The notion of a local inertial reference frame is thoroughly analyzed. Dynamics of a field of such frames is derived from the variational principle. It is shown that the resulting theory splits naturally into three sectors, one of which is purely gravitational. Field dynamics in this sector, equivalent to Einstein&amp;amp;rsquo;s vacuum equations, is obtained unambiguously and admits no ad hoc corrections. The cosmological constant is an essential element of this construction and cannot be removed. It has been shown that the second sector of this theory corresponds to electrodynamics, while the last sector could possibly describe dark matter.</p>
	]]></content:encoded>

	<dc:title>Gravity on a Large Scale&amp;amp;mdash;Does It Necessarily Look like It Does on a Small Scale?</dc:title>
			<dc:creator>Jerzy Kijowski</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3010004</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-03-01</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-03-01</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>29</prism:startingPage>
		<prism:doi>10.3390/astronomy3010004</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/1/3">

	<title>Astronomy, Vol. 3, Pages 21-28: Possible Tests of Fundamental Physics with GINGER</title>
	<link>https://www.mdpi.com/2674-0346/3/1/3</link>
	<description>The GINGER (gyroscopes in general relativity) project foresees the construction of an array of large frame ring laser gyroscopes, rigidly connected to the Earth. Large frame ring laser gyroscopes are high-sensitivity instruments used to measure angular velocity with respect to the local inertial frame. In particular, they can provide sub-daily variations in the Earth rotation rate, a measurement relevant for geodesy and for fundamental physics at the same time. Sensitivity is the key point in determining the relevance of this instrument for fundamental science. The most recent progress in sensitivity evaluation, obtained on a ring laser prototype, indicates that GINGER should reach the level of 1 part in 1011 of the Earth&amp;amp;rsquo;s rotation rate. The impact on fundamental physics of this kind of apparatus is reviewed.</description>
	<pubDate>2024-02-29</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 21-28: Possible Tests of Fundamental Physics with GINGER</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/1/3">doi: 10.3390/astronomy3010003</a></p>
	<p>Authors:
		Giuseppe Di Somma
		Carlo Altucci
		Francesco Bajardi
		Andrea Basti
		Nicolò Beverini
		Salvatore Capozziello
		Giorgio Carelli
		Simone Castellano
		Donatella Ciampini
		Gaetano De Luca
		Angela D. V. Di Virgilio
		Francesco Fuso
		Francesco Giovinetti
		Enrico Maccioni
		Paolo Marsili
		Antonello Ortolan
		Alberto Porzio
		Matteo Luca Ruggiero
		Raffaele Velotta
		</p>
	<p>The GINGER (gyroscopes in general relativity) project foresees the construction of an array of large frame ring laser gyroscopes, rigidly connected to the Earth. Large frame ring laser gyroscopes are high-sensitivity instruments used to measure angular velocity with respect to the local inertial frame. In particular, they can provide sub-daily variations in the Earth rotation rate, a measurement relevant for geodesy and for fundamental physics at the same time. Sensitivity is the key point in determining the relevance of this instrument for fundamental science. The most recent progress in sensitivity evaluation, obtained on a ring laser prototype, indicates that GINGER should reach the level of 1 part in 1011 of the Earth&amp;amp;rsquo;s rotation rate. The impact on fundamental physics of this kind of apparatus is reviewed.</p>
	]]></content:encoded>

	<dc:title>Possible Tests of Fundamental Physics with GINGER</dc:title>
			<dc:creator>Giuseppe Di Somma</dc:creator>
			<dc:creator>Carlo Altucci</dc:creator>
			<dc:creator>Francesco Bajardi</dc:creator>
			<dc:creator>Andrea Basti</dc:creator>
			<dc:creator>Nicolò Beverini</dc:creator>
			<dc:creator>Salvatore Capozziello</dc:creator>
			<dc:creator>Giorgio Carelli</dc:creator>
			<dc:creator>Simone Castellano</dc:creator>
			<dc:creator>Donatella Ciampini</dc:creator>
			<dc:creator>Gaetano De Luca</dc:creator>
			<dc:creator>Angela D. V. Di Virgilio</dc:creator>
			<dc:creator>Francesco Fuso</dc:creator>
			<dc:creator>Francesco Giovinetti</dc:creator>
			<dc:creator>Enrico Maccioni</dc:creator>
			<dc:creator>Paolo Marsili</dc:creator>
			<dc:creator>Antonello Ortolan</dc:creator>
			<dc:creator>Alberto Porzio</dc:creator>
			<dc:creator>Matteo Luca Ruggiero</dc:creator>
			<dc:creator>Raffaele Velotta</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3010003</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-02-29</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-02-29</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Brief Report</prism:section>
	<prism:startingPage>21</prism:startingPage>
		<prism:doi>10.3390/astronomy3010003</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/1/2">

	<title>Astronomy, Vol. 3, Pages 14-20: Beyond mirkwood: Enhancing SED Modeling with Conformal Predictions</title>
	<link>https://www.mdpi.com/2674-0346/3/1/2</link>
	<description>Traditional spectral energy distribution (SED) fitting techniques face uncertainties due to assumptions in star formation histories and dust attenuation curves. We propose an advanced machine learning-based approach that enhances flexibility and uncertainty quantification in SED fitting. Unlike the fixed NGBoost model used in mirkwood, our approach allows for any scikit-learn-compatible model, including deterministic models. We incorporate conformalized quantile regression to convert point predictions into error bars, enhancing interpretability and reliability. Using CatBoost as the base predictor, we compare results with and without conformal prediction, demonstrating improved performance using metrics such as coverage and interval width. Our method offers a more versatile and accurate tool for deriving galaxy physical properties from observational data.</description>
	<pubDate>2024-02-10</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 14-20: Beyond mirkwood: Enhancing SED Modeling with Conformal Predictions</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/1/2">doi: 10.3390/astronomy3010002</a></p>
	<p>Authors:
		Sankalp Gilda
		</p>
	<p>Traditional spectral energy distribution (SED) fitting techniques face uncertainties due to assumptions in star formation histories and dust attenuation curves. We propose an advanced machine learning-based approach that enhances flexibility and uncertainty quantification in SED fitting. Unlike the fixed NGBoost model used in mirkwood, our approach allows for any scikit-learn-compatible model, including deterministic models. We incorporate conformalized quantile regression to convert point predictions into error bars, enhancing interpretability and reliability. Using CatBoost as the base predictor, we compare results with and without conformal prediction, demonstrating improved performance using metrics such as coverage and interval width. Our method offers a more versatile and accurate tool for deriving galaxy physical properties from observational data.</p>
	]]></content:encoded>

	<dc:title>Beyond mirkwood: Enhancing SED Modeling with Conformal Predictions</dc:title>
			<dc:creator>Sankalp Gilda</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3010002</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-02-10</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-02-10</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Conference Report</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/astronomy3010002</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/3/1/1">

	<title>Astronomy, Vol. 3, Pages 1-13: Generating Stellar Spectra Using Neural Networks</title>
	<link>https://www.mdpi.com/2674-0346/3/1/1</link>
	<description>A new generative technique is presented in this paper that uses Deep Learning to reconstruct stellar spectra based on a set of stellar parameters. Two different Neural Networks were trained allowing the generation of new spectra. First, an autoencoder is trained on a set of BAFGK synthetic data calculated using ATLAS9 model atmospheres and SYNSPEC radiative transfer code. These spectra are calculated in the wavelength range of Gaia RVS between 8400 and 8800 &amp;amp;Aring;. Second, we trained a Fully Dense Neural Network to relate the stellar parameters to the Latent Space of the autoencoder. Finally, we linked the Fully Dense Neural Network to the decoder part of the autoencoder and we built a model that uses as input any combination of Teff, logg, vesini, [M/H], and &amp;amp;xi;t and output a normalized spectrum. The generated spectra are shown to represent all the line profiles and flux values as the ones calculated using the classical radiative transfer code. The accuracy of our technique is tested using a stellar parameter determination procedure and the results show that the generated spectra have the same characteristics as the synthetic ones.</description>
	<pubDate>2024-01-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 3, Pages 1-13: Generating Stellar Spectra Using Neural Networks</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/3/1/1">doi: 10.3390/astronomy3010001</a></p>
	<p>Authors:
		Marwan Gebran
		</p>
	<p>A new generative technique is presented in this paper that uses Deep Learning to reconstruct stellar spectra based on a set of stellar parameters. Two different Neural Networks were trained allowing the generation of new spectra. First, an autoencoder is trained on a set of BAFGK synthetic data calculated using ATLAS9 model atmospheres and SYNSPEC radiative transfer code. These spectra are calculated in the wavelength range of Gaia RVS between 8400 and 8800 &amp;amp;Aring;. Second, we trained a Fully Dense Neural Network to relate the stellar parameters to the Latent Space of the autoencoder. Finally, we linked the Fully Dense Neural Network to the decoder part of the autoencoder and we built a model that uses as input any combination of Teff, logg, vesini, [M/H], and &amp;amp;xi;t and output a normalized spectrum. The generated spectra are shown to represent all the line profiles and flux values as the ones calculated using the classical radiative transfer code. The accuracy of our technique is tested using a stellar parameter determination procedure and the results show that the generated spectra have the same characteristics as the synthetic ones.</p>
	]]></content:encoded>

	<dc:title>Generating Stellar Spectra Using Neural Networks</dc:title>
			<dc:creator>Marwan Gebran</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy3010001</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2024-01-30</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2024-01-30</prism:publicationDate>
	<prism:volume>3</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Technical Note</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/astronomy3010001</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/3/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/4/20">

	<title>Astronomy, Vol. 2, Pages 300-314: Testing Cosmic Acceleration from the Late-Time Universe</title>
	<link>https://www.mdpi.com/2674-0346/2/4/20</link>
	<description>We investigate the accelerated cosmic expansion in the late universe and derive constraints on the values of the cosmic key parameters according to different cosmologies such as &amp;amp;Lambda;CDM, wCDM, and w0waCDM. We select 24 baryon acoustic oscillation (BAO) uncorrelated measurements from the latest galaxy surveys measurements in the range of redshift z&amp;amp;isin;[0.106,2.33] combined with the Pantheon SNeIa dataset, the latest 33 H(z) measurements using the cosmic chronometers (CCs) method, and the recent Hubble constant value measurement measured by Riess 2022 (R22) as an additional prior. In the &amp;amp;Lambda;CDM framework, the model fit yields &amp;amp;Omega;m=0.268&amp;amp;plusmn;0.037 and &amp;amp;Omega;&amp;amp;Lambda;=0.726&amp;amp;plusmn;0.023. Combining BAO with Pantheon plus the cosmic chronometers datasets we obtain H0=69.76&amp;amp;plusmn;1.71 km s&amp;amp;minus;1 Mpc&amp;amp;minus;1 and the sound horizon result is rd=145.88&amp;amp;plusmn;3.32 Mpc. For the flat wCDM model, we obtain w=&amp;amp;minus;1.001&amp;amp;plusmn;0.040. For the dynamical evolution of the dark energy equation of state, w0waCDM cosmology, we obtain wa=&amp;amp;minus;0.848&amp;amp;plusmn;0.180. We apply the Akaike information criterion approach to compare the three models, and see that all cannot be ruled out from the latest observational measurements.</description>
	<pubDate>2023-12-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 300-314: Testing Cosmic Acceleration from the Late-Time Universe</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/4/20">doi: 10.3390/astronomy2040020</a></p>
	<p>Authors:
		Jose Agustin Lozano Torres
		</p>
	<p>We investigate the accelerated cosmic expansion in the late universe and derive constraints on the values of the cosmic key parameters according to different cosmologies such as &amp;amp;Lambda;CDM, wCDM, and w0waCDM. We select 24 baryon acoustic oscillation (BAO) uncorrelated measurements from the latest galaxy surveys measurements in the range of redshift z&amp;amp;isin;[0.106,2.33] combined with the Pantheon SNeIa dataset, the latest 33 H(z) measurements using the cosmic chronometers (CCs) method, and the recent Hubble constant value measurement measured by Riess 2022 (R22) as an additional prior. In the &amp;amp;Lambda;CDM framework, the model fit yields &amp;amp;Omega;m=0.268&amp;amp;plusmn;0.037 and &amp;amp;Omega;&amp;amp;Lambda;=0.726&amp;amp;plusmn;0.023. Combining BAO with Pantheon plus the cosmic chronometers datasets we obtain H0=69.76&amp;amp;plusmn;1.71 km s&amp;amp;minus;1 Mpc&amp;amp;minus;1 and the sound horizon result is rd=145.88&amp;amp;plusmn;3.32 Mpc. For the flat wCDM model, we obtain w=&amp;amp;minus;1.001&amp;amp;plusmn;0.040. For the dynamical evolution of the dark energy equation of state, w0waCDM cosmology, we obtain wa=&amp;amp;minus;0.848&amp;amp;plusmn;0.180. We apply the Akaike information criterion approach to compare the three models, and see that all cannot be ruled out from the latest observational measurements.</p>
	]]></content:encoded>

	<dc:title>Testing Cosmic Acceleration from the Late-Time Universe</dc:title>
			<dc:creator>Jose Agustin Lozano Torres</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2040020</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-12-14</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-12-14</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>300</prism:startingPage>
		<prism:doi>10.3390/astronomy2040020</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/4/20</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/4/19">

	<title>Astronomy, Vol. 2, Pages 286-299: Frequency&amp;ndash;Redshift Relation of the Cosmic Microwave Background</title>
	<link>https://www.mdpi.com/2674-0346/2/4/19</link>
	<description>We point out that a modified temperature&amp;amp;ndash;redshift relation (T-z relation) of the cosmic microwave background (CMB) cannot be deduced by any observational method that appeals to an a priori thermalisation to the CMB temperature T of the excited states in a probe environment of independently determined redshift z. For example, this applies to quasar-light absorption by a damped Lyman-alpha system due to atomic as well as ionic fine-splitting transitions or molecular rotational bands. Similarly, the thermal Sunyaev-Zel&amp;amp;rsquo;dovich (thSZ) effect cannot be used to extract the CMB&amp;amp;rsquo;s T-z relation. This is because the relative line strengths between ground and excited states in the former and the CMB spectral distortion in the latter case both depend, apart from environment-specific normalisations, solely on the dimensionless spectral variable x=h&amp;amp;nu;kBT. Since the literature on extractions of the CMB&amp;amp;rsquo;s T-z relation always assumes (i) &amp;amp;nu;(z)=(1+z)&amp;amp;nu;(z=0), where &amp;amp;nu;(z=0) is the observed frequency in the heliocentric rest frame, the finding (ii) T(z)=(1+z)T(z=0) just confirms the expected blackbody nature of the interacting CMB at z&amp;amp;gt;0. In contrast to the emission of isolated, directed radiation, whose frequency&amp;amp;ndash;redshift relation (&amp;amp;nu;-z relation) is subject to (i), a non-conventional &amp;amp;nu;-z relation &amp;amp;nu;(z)=f(z)&amp;amp;nu;(z=0) of pure, isotropic blackbody radiation, subject to adiabatically slow cosmic expansion, necessarily has to follow that of the T-z relation T(z)=f(z)T(z=0) and vice versa. In general, the function f(z) is determined by the energy conservation of the CMB fluid in a Friedmann&amp;amp;ndash;Lemaitre&amp;amp;ndash;Robertson&amp;amp;ndash;Walker universe. If the pure CMB is subject to an SU(2) rather than a U(1) gauge principle, then f(z)=1/41/3(1+z) for z&amp;amp;#8811;1, and f(z) is non-linear for z&amp;amp;sim;1.</description>
	<pubDate>2023-11-08</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 286-299: Frequency&amp;ndash;Redshift Relation of the Cosmic Microwave Background</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/4/19">doi: 10.3390/astronomy2040019</a></p>
	<p>Authors:
		Ralf Hofmann
		Janning Meinert
		</p>
	<p>We point out that a modified temperature&amp;amp;ndash;redshift relation (T-z relation) of the cosmic microwave background (CMB) cannot be deduced by any observational method that appeals to an a priori thermalisation to the CMB temperature T of the excited states in a probe environment of independently determined redshift z. For example, this applies to quasar-light absorption by a damped Lyman-alpha system due to atomic as well as ionic fine-splitting transitions or molecular rotational bands. Similarly, the thermal Sunyaev-Zel&amp;amp;rsquo;dovich (thSZ) effect cannot be used to extract the CMB&amp;amp;rsquo;s T-z relation. This is because the relative line strengths between ground and excited states in the former and the CMB spectral distortion in the latter case both depend, apart from environment-specific normalisations, solely on the dimensionless spectral variable x=h&amp;amp;nu;kBT. Since the literature on extractions of the CMB&amp;amp;rsquo;s T-z relation always assumes (i) &amp;amp;nu;(z)=(1+z)&amp;amp;nu;(z=0), where &amp;amp;nu;(z=0) is the observed frequency in the heliocentric rest frame, the finding (ii) T(z)=(1+z)T(z=0) just confirms the expected blackbody nature of the interacting CMB at z&amp;amp;gt;0. In contrast to the emission of isolated, directed radiation, whose frequency&amp;amp;ndash;redshift relation (&amp;amp;nu;-z relation) is subject to (i), a non-conventional &amp;amp;nu;-z relation &amp;amp;nu;(z)=f(z)&amp;amp;nu;(z=0) of pure, isotropic blackbody radiation, subject to adiabatically slow cosmic expansion, necessarily has to follow that of the T-z relation T(z)=f(z)T(z=0) and vice versa. In general, the function f(z) is determined by the energy conservation of the CMB fluid in a Friedmann&amp;amp;ndash;Lemaitre&amp;amp;ndash;Robertson&amp;amp;ndash;Walker universe. If the pure CMB is subject to an SU(2) rather than a U(1) gauge principle, then f(z)=1/41/3(1+z) for z&amp;amp;#8811;1, and f(z) is non-linear for z&amp;amp;sim;1.</p>
	]]></content:encoded>

	<dc:title>Frequency&amp;amp;ndash;Redshift Relation of the Cosmic Microwave Background</dc:title>
			<dc:creator>Ralf Hofmann</dc:creator>
			<dc:creator>Janning Meinert</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2040019</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-11-08</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-11-08</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>286</prism:startingPage>
		<prism:doi>10.3390/astronomy2040019</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/4/19</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/4/18">

	<title>Astronomy, Vol. 2, Pages 269-285: Schwarzschild Black Holes in Extended Spacetime with Two Time Dimensions</title>
	<link>https://www.mdpi.com/2674-0346/2/4/18</link>
	<description>Black holes are one of the most extreme phenomena in the Universe, bridging the gap between the realms of general relativity and quantum physics. Any matter that crosses the event horizon moves towards the core of the black hole, creating a singularity with infinite mass density&amp;amp;mdash;a phenomenon that cannot be comprehended within present theories of relativity and quantum physics. In this study, we undertake an investigation of non-rotating, non-charged Schwarzschild black holes in an extended spacetime framework with two time dimensions. To accomplish this, we extend Einstein&amp;amp;rsquo;s field equations by one more temporal dimension. We solve the corresponding equations for a spherical central mass, which leads to an Abel-type equation for the 5D Schwarzschild metric. By exploring distinct solution classes, we present an approximate solution for the 5D metric. Our proposed solution maintains consistency with Schwarzschild&amp;amp;rsquo;s 4D solution. Finally, we address the central black hole singularity and demonstrate a potential breakthrough, as our solution effectively avoids the singularity quandary, providing valuable insight into the fundamental properties of black holes in this augmented framework.</description>
	<pubDate>2023-11-06</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 269-285: Schwarzschild Black Holes in Extended Spacetime with Two Time Dimensions</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/4/18">doi: 10.3390/astronomy2040018</a></p>
	<p>Authors:
		Mechid Paiman
		Horia Cornean
		Christoph Köhn
		</p>
	<p>Black holes are one of the most extreme phenomena in the Universe, bridging the gap between the realms of general relativity and quantum physics. Any matter that crosses the event horizon moves towards the core of the black hole, creating a singularity with infinite mass density&amp;amp;mdash;a phenomenon that cannot be comprehended within present theories of relativity and quantum physics. In this study, we undertake an investigation of non-rotating, non-charged Schwarzschild black holes in an extended spacetime framework with two time dimensions. To accomplish this, we extend Einstein&amp;amp;rsquo;s field equations by one more temporal dimension. We solve the corresponding equations for a spherical central mass, which leads to an Abel-type equation for the 5D Schwarzschild metric. By exploring distinct solution classes, we present an approximate solution for the 5D metric. Our proposed solution maintains consistency with Schwarzschild&amp;amp;rsquo;s 4D solution. Finally, we address the central black hole singularity and demonstrate a potential breakthrough, as our solution effectively avoids the singularity quandary, providing valuable insight into the fundamental properties of black holes in this augmented framework.</p>
	]]></content:encoded>

	<dc:title>Schwarzschild Black Holes in Extended Spacetime with Two Time Dimensions</dc:title>
			<dc:creator>Mechid Paiman</dc:creator>
			<dc:creator>Horia Cornean</dc:creator>
			<dc:creator>Christoph Köhn</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2040018</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-11-06</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-11-06</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>269</prism:startingPage>
		<prism:doi>10.3390/astronomy2040018</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/4/18</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/4/17">

	<title>Astronomy, Vol. 2, Pages 235-268: The Upgraded Planck System of Units That Reaches from the Known Planck Scale All the Way Down to Subatomic Scales</title>
	<link>https://www.mdpi.com/2674-0346/2/4/17</link>
	<description>Natural systems of units {Ui} need to be overhauled to include the dimensionless coupling constants {&amp;amp;alpha;Ui} of the natural forces. Otherwise, they cannot quantify all the forces of nature in a unified manner. Thus, each force must furnish a system of units with at least one dimensional and one dimensionless constant. We revisit three natural systems of units (atomic, cosmological, and Planck). The Planck system is easier to rectify, and we do so in this work. The atomic system discounts {G,&amp;amp;alpha;G}, thus it cannot account for gravitation. The cosmological system discounts {h,&amp;amp;alpha;h}, thus it cannot account for quantum physics. Here, the symbols have their usual meanings; in particular, &amp;amp;alpha;G is the gravitational coupling constant and &amp;amp;alpha;h is Dirac&amp;amp;rsquo;s fine-structure constant. The speed of light c and the impedance of free space Z0 are resistive properties imposed by the vacuum itself; thus, they must be present in all systems of units. The upgraded Planck system with fundamental units UPS:={c,Z0,G,&amp;amp;alpha;G,h,&amp;amp;alpha;h,&amp;amp;hellip;} describes all physical scales in the universe&amp;amp;mdash;it is nature&amp;amp;rsquo;s system of units. As such, it reveals a number of properties, most of which have been encountered previously in seemingly disjoint parts of physics and some of which have been designated as mere coincidences. Based on the UPS results, which relate (sub)atomic scales to the Planck scale and the fine-structure constant to the Higgs field, we can state with confidence that no observed or measured physical properties are coincidental in this universe. Furthermore, we derive from first principles Koide&amp;amp;rsquo;s K=2/3 enigmatic constant and additional analogous quark and vector boson constants. These are formal mathematical proofs that justify a posteriori the use of geometric means in deriving the quark/boson mass ladder. This ladder allows us to also calculate the Higgs couplings to the vector bosons and the Weinberg angle in terms of K only, and many of the &amp;amp;ldquo;free&amp;amp;rdquo; parameters of the Standard Model of particle physics were previously expected to be determined only from experiments.</description>
	<pubDate>2023-10-30</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 235-268: The Upgraded Planck System of Units That Reaches from the Known Planck Scale All the Way Down to Subatomic Scales</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/4/17">doi: 10.3390/astronomy2040017</a></p>
	<p>Authors:
		Dimitris M. Christodoulou
		Demosthenes Kazanas
		</p>
	<p>Natural systems of units {Ui} need to be overhauled to include the dimensionless coupling constants {&amp;amp;alpha;Ui} of the natural forces. Otherwise, they cannot quantify all the forces of nature in a unified manner. Thus, each force must furnish a system of units with at least one dimensional and one dimensionless constant. We revisit three natural systems of units (atomic, cosmological, and Planck). The Planck system is easier to rectify, and we do so in this work. The atomic system discounts {G,&amp;amp;alpha;G}, thus it cannot account for gravitation. The cosmological system discounts {h,&amp;amp;alpha;h}, thus it cannot account for quantum physics. Here, the symbols have their usual meanings; in particular, &amp;amp;alpha;G is the gravitational coupling constant and &amp;amp;alpha;h is Dirac&amp;amp;rsquo;s fine-structure constant. The speed of light c and the impedance of free space Z0 are resistive properties imposed by the vacuum itself; thus, they must be present in all systems of units. The upgraded Planck system with fundamental units UPS:={c,Z0,G,&amp;amp;alpha;G,h,&amp;amp;alpha;h,&amp;amp;hellip;} describes all physical scales in the universe&amp;amp;mdash;it is nature&amp;amp;rsquo;s system of units. As such, it reveals a number of properties, most of which have been encountered previously in seemingly disjoint parts of physics and some of which have been designated as mere coincidences. Based on the UPS results, which relate (sub)atomic scales to the Planck scale and the fine-structure constant to the Higgs field, we can state with confidence that no observed or measured physical properties are coincidental in this universe. Furthermore, we derive from first principles Koide&amp;amp;rsquo;s K=2/3 enigmatic constant and additional analogous quark and vector boson constants. These are formal mathematical proofs that justify a posteriori the use of geometric means in deriving the quark/boson mass ladder. This ladder allows us to also calculate the Higgs couplings to the vector bosons and the Weinberg angle in terms of K only, and many of the &amp;amp;ldquo;free&amp;amp;rdquo; parameters of the Standard Model of particle physics were previously expected to be determined only from experiments.</p>
	]]></content:encoded>

	<dc:title>The Upgraded Planck System of Units That Reaches from the Known Planck Scale All the Way Down to Subatomic Scales</dc:title>
			<dc:creator>Dimitris M. Christodoulou</dc:creator>
			<dc:creator>Demosthenes Kazanas</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2040017</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-10-30</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-10-30</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>235</prism:startingPage>
		<prism:doi>10.3390/astronomy2040017</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/4/17</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/4/16">

	<title>Astronomy, Vol. 2, Pages 226-234: Radio Pulsars Resonantly Accelerating Electrons</title>
	<link>https://www.mdpi.com/2674-0346/2/4/16</link>
	<description>Based on the recently demonstrated resonant wave&amp;amp;ndash;wave process, it is shown that electrons can be accelerated to ultra-relativistic energies in the magnetospheres of radio pulsars. The energization occurs via the resonant interaction of the electron wave (described by the Klein&amp;amp;ndash;Gordon (KG) equation) moving in unison with an intense electromagnetic (EM) wave; the KG wave/particle continuously draws energy from EM. In a brief recapitulation of the general theory, the high-energy (resonantly enhanced) electron states are investigated by solving the KG equation, minimally coupled to the EM field. The restricted class of solutions that propagate in phase with EM radiation (functions only of &amp;amp;zeta;=&amp;amp;omega;t&amp;amp;minus;kz) are explored to serve as a possible basis for the proposed electron energization in the radio pulsars. We show that the wave&amp;amp;ndash;wave resonant energization mechanism could be operative in a broad class of radio pulsars with periods ranging from milliseconds to normal values (&amp;amp;sim;1 s); this could drive the magnetospheric electrons to acquire energies from 100 s of TeVs (millisecond pulsars) to 10 ZeVs (normal pulsars).</description>
	<pubDate>2023-10-13</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 226-234: Radio Pulsars Resonantly Accelerating Electrons</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/4/16">doi: 10.3390/astronomy2040016</a></p>
	<p>Authors:
		Zaza N. Osmanov
		Swadesh M. Mahajan
		</p>
	<p>Based on the recently demonstrated resonant wave&amp;amp;ndash;wave process, it is shown that electrons can be accelerated to ultra-relativistic energies in the magnetospheres of radio pulsars. The energization occurs via the resonant interaction of the electron wave (described by the Klein&amp;amp;ndash;Gordon (KG) equation) moving in unison with an intense electromagnetic (EM) wave; the KG wave/particle continuously draws energy from EM. In a brief recapitulation of the general theory, the high-energy (resonantly enhanced) electron states are investigated by solving the KG equation, minimally coupled to the EM field. The restricted class of solutions that propagate in phase with EM radiation (functions only of &amp;amp;zeta;=&amp;amp;omega;t&amp;amp;minus;kz) are explored to serve as a possible basis for the proposed electron energization in the radio pulsars. We show that the wave&amp;amp;ndash;wave resonant energization mechanism could be operative in a broad class of radio pulsars with periods ranging from milliseconds to normal values (&amp;amp;sim;1 s); this could drive the magnetospheric electrons to acquire energies from 100 s of TeVs (millisecond pulsars) to 10 ZeVs (normal pulsars).</p>
	]]></content:encoded>

	<dc:title>Radio Pulsars Resonantly Accelerating Electrons</dc:title>
			<dc:creator>Zaza N. Osmanov</dc:creator>
			<dc:creator>Swadesh M. Mahajan</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2040016</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-10-13</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-10-13</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>4</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>226</prism:startingPage>
		<prism:doi>10.3390/astronomy2040016</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/4/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/15">

	<title>Astronomy, Vol. 2, Pages 206-225: Emergent Strings at an Infinite Distance with Broken Supersymmetry</title>
	<link>https://www.mdpi.com/2674-0346/2/3/15</link>
	<description>We investigate the infinite-distance properties of families of unstable flux vacua in string theory with broken supersymmetry. To this end, we employ a generalized notion of distance in the moduli space and we build a holographic description for the non-perturbative regime of the tunneling cascade in terms of a renormalization group flow. In one limit, we recover an exponentially-light tower of Kaluza-Klein states, while in the opposite limit, we find a tower of higher-spin excitations of D1-branes, realizing the emergent string proposal. In particular, the holographic description includes a free sector, whose emergent superconformal symmetry resonates with supersymmetric stability, the CFT distance conjecture and S-duality. We compute the anomalous dimensions of scalar vertex operators and single-trace higher-spin currents, finding an exponential suppression with the distance which is not generic from the renormalization group perspective, but appears specific to our settings.</description>
	<pubDate>2023-09-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 206-225: Emergent Strings at an Infinite Distance with Broken Supersymmetry</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/15">doi: 10.3390/astronomy2030015</a></p>
	<p>Authors:
		Ivano Basile
		</p>
	<p>We investigate the infinite-distance properties of families of unstable flux vacua in string theory with broken supersymmetry. To this end, we employ a generalized notion of distance in the moduli space and we build a holographic description for the non-perturbative regime of the tunneling cascade in terms of a renormalization group flow. In one limit, we recover an exponentially-light tower of Kaluza-Klein states, while in the opposite limit, we find a tower of higher-spin excitations of D1-branes, realizing the emergent string proposal. In particular, the holographic description includes a free sector, whose emergent superconformal symmetry resonates with supersymmetric stability, the CFT distance conjecture and S-duality. We compute the anomalous dimensions of scalar vertex operators and single-trace higher-spin currents, finding an exponential suppression with the distance which is not generic from the renormalization group perspective, but appears specific to our settings.</p>
	]]></content:encoded>

	<dc:title>Emergent Strings at an Infinite Distance with Broken Supersymmetry</dc:title>
			<dc:creator>Ivano Basile</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030015</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-09-14</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-09-14</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>206</prism:startingPage>
		<prism:doi>10.3390/astronomy2030015</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/14">

	<title>Astronomy, Vol. 2, Pages 193-205: New Strong Constraints on the Central Behaviour of Spherical Galactic Models</title>
	<link>https://www.mdpi.com/2674-0346/2/3/14</link>
	<description>First of all, we show that any spherically symmetric galactic model with integrated mass profile M(r)&amp;amp;rarr;0 as r&amp;amp;rarr;0 is physically correct close to the centre only provided that the circular velocity vc(r)&amp;amp;rarr;0 and the gravitational field g(r)&amp;amp;rarr;0 as r&amp;amp;rarr;0. Next, we apply this statement to a broad class of five-parameter spherical galactic models, including most of those used in astrophysics and cosmology. Specifically, we show that the Jaffe and Hernquist models can be trusted only for r&amp;amp;#8819;0.2Re (Re being the effective radius), while the Navarro&amp;amp;ndash;Frank&amp;amp;ndash;White (NFW) model cannot describe galaxies in the central region of regular clusters. We also briefly discuss the relevance of our result for the NFW profile of pure dark matter halos. However, we are unable to tell at which central distance the NFW model breaks down in either case, and this is a challenge for future investigations.</description>
	<pubDate>2023-09-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 193-205: New Strong Constraints on the Central Behaviour of Spherical Galactic Models</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/14">doi: 10.3390/astronomy2030014</a></p>
	<p>Authors:
		Marco Roncadelli
		Giorgio Galanti
		</p>
	<p>First of all, we show that any spherically symmetric galactic model with integrated mass profile M(r)&amp;amp;rarr;0 as r&amp;amp;rarr;0 is physically correct close to the centre only provided that the circular velocity vc(r)&amp;amp;rarr;0 and the gravitational field g(r)&amp;amp;rarr;0 as r&amp;amp;rarr;0. Next, we apply this statement to a broad class of five-parameter spherical galactic models, including most of those used in astrophysics and cosmology. Specifically, we show that the Jaffe and Hernquist models can be trusted only for r&amp;amp;#8819;0.2Re (Re being the effective radius), while the Navarro&amp;amp;ndash;Frank&amp;amp;ndash;White (NFW) model cannot describe galaxies in the central region of regular clusters. We also briefly discuss the relevance of our result for the NFW profile of pure dark matter halos. However, we are unable to tell at which central distance the NFW model breaks down in either case, and this is a challenge for future investigations.</p>
	]]></content:encoded>

	<dc:title>New Strong Constraints on the Central Behaviour of Spherical Galactic Models</dc:title>
			<dc:creator>Marco Roncadelli</dc:creator>
			<dc:creator>Giorgio Galanti</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030014</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-09-01</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-09-01</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>193</prism:startingPage>
		<prism:doi>10.3390/astronomy2030014</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/13">

	<title>Astronomy, Vol. 2, Pages 180-192: Quantum Astronomy at the University and INAF Astronomical Observatory of Padova, Italy</title>
	<link>https://www.mdpi.com/2674-0346/2/3/13</link>
	<description>Twenty years ago, we started to apply quantum optics to the astronomical research carried out inside the Department of Physics and Astronomy and the INAF Astronomical Observatory in Padova, Italy. The initial activities were stimulated by the project of the European Southern Observatory (ESO) to build a 100 m diameter telescope, the Overwhelmingly Large (OWL) telescope. The enormous photon flux expected from such an aperture suggested that quantum optics concepts be utilized in order to obtain novel astrophysical results. Following initial successful attempts to utilize the orbital angular momentum of the light beam to enhance the visibility of faint companions to bright stars, the Padova team concentrated its efforts on very high time resolution, in order to measure and store the arrival time of celestial photons to better than one nanosecond. To obtain observational results, we built two photon counting photometers (AquEye and IquEye) to be used with our telescopes of the Asiago Observatory and with 4 m class telescopes such as the ESO New Technology Telescope (NTT) in Chile. This paper firstly describes these two instruments and then expounds the results obtained on pulsar light curves, lunar occultations and the first photon counting intensity interferometry measurements of the bright star Vega. Indeed, the correlation of photon arrival times on two or more apertures can lead to extremely high angular resolutions, as shown around 1970 by Hanbury Brown and Twiss. Prospects for quantum intensity interferometry with arrays of Cherenkov light telescopes will also be described.</description>
	<pubDate>2023-08-23</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 180-192: Quantum Astronomy at the University and INAF Astronomical Observatory of Padova, Italy</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/13">doi: 10.3390/astronomy2030013</a></p>
	<p>Authors:
		Cesare Barbieri
		Giampiero Naletto
		Luca Zampieri
		</p>
	<p>Twenty years ago, we started to apply quantum optics to the astronomical research carried out inside the Department of Physics and Astronomy and the INAF Astronomical Observatory in Padova, Italy. The initial activities were stimulated by the project of the European Southern Observatory (ESO) to build a 100 m diameter telescope, the Overwhelmingly Large (OWL) telescope. The enormous photon flux expected from such an aperture suggested that quantum optics concepts be utilized in order to obtain novel astrophysical results. Following initial successful attempts to utilize the orbital angular momentum of the light beam to enhance the visibility of faint companions to bright stars, the Padova team concentrated its efforts on very high time resolution, in order to measure and store the arrival time of celestial photons to better than one nanosecond. To obtain observational results, we built two photon counting photometers (AquEye and IquEye) to be used with our telescopes of the Asiago Observatory and with 4 m class telescopes such as the ESO New Technology Telescope (NTT) in Chile. This paper firstly describes these two instruments and then expounds the results obtained on pulsar light curves, lunar occultations and the first photon counting intensity interferometry measurements of the bright star Vega. Indeed, the correlation of photon arrival times on two or more apertures can lead to extremely high angular resolutions, as shown around 1970 by Hanbury Brown and Twiss. Prospects for quantum intensity interferometry with arrays of Cherenkov light telescopes will also be described.</p>
	]]></content:encoded>

	<dc:title>Quantum Astronomy at the University and INAF Astronomical Observatory of Padova, Italy</dc:title>
			<dc:creator>Cesare Barbieri</dc:creator>
			<dc:creator>Giampiero Naletto</dc:creator>
			<dc:creator>Luca Zampieri</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030013</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-08-23</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-08-23</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>180</prism:startingPage>
		<prism:doi>10.3390/astronomy2030013</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/12">

	<title>Astronomy, Vol. 2, Pages 165-179: Space Weather Effects on Satellites</title>
	<link>https://www.mdpi.com/2674-0346/2/3/12</link>
	<description>The study presents a concise overview on the main effects on satellites due to space weather drivers compared to the well-known interplanetary, magnetospheric and ground-based consequences. The solar-activity-driven influences include specific physics-based effects on the spacecraft surface and on-board electronics due to electromagnetic emission and energetic particles as well as complex effects due to geomagnetic storms which may endanger the mission performance and spacecraft longevity. We select as test examples the Starlink satellites in the period 2019&amp;amp;ndash;2022 and present the temporal correspondence between their launches and the space weather phenomena. Based on comparative analysis, we discuss whether the occurrence vs. the intensity of solar and interplanetary drivers of space weather can be considered as a cause for orbital stability problems and satellite loss. The results suggest that a sequence of geomagnetic disturbances together with multiple weak space weather events could lead to severe levels of atmospheric drag ending in a service or satellite loss.</description>
	<pubDate>2023-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 165-179: Space Weather Effects on Satellites</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/12">doi: 10.3390/astronomy2030012</a></p>
	<p>Authors:
		Rositsa Miteva
		Susan W. Samwel
		Stela Tkatchova
		</p>
	<p>The study presents a concise overview on the main effects on satellites due to space weather drivers compared to the well-known interplanetary, magnetospheric and ground-based consequences. The solar-activity-driven influences include specific physics-based effects on the spacecraft surface and on-board electronics due to electromagnetic emission and energetic particles as well as complex effects due to geomagnetic storms which may endanger the mission performance and spacecraft longevity. We select as test examples the Starlink satellites in the period 2019&amp;amp;ndash;2022 and present the temporal correspondence between their launches and the space weather phenomena. Based on comparative analysis, we discuss whether the occurrence vs. the intensity of solar and interplanetary drivers of space weather can be considered as a cause for orbital stability problems and satellite loss. The results suggest that a sequence of geomagnetic disturbances together with multiple weak space weather events could lead to severe levels of atmospheric drag ending in a service or satellite loss.</p>
	]]></content:encoded>

	<dc:title>Space Weather Effects on Satellites</dc:title>
			<dc:creator>Rositsa Miteva</dc:creator>
			<dc:creator>Susan W. Samwel</dc:creator>
			<dc:creator>Stela Tkatchova</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030012</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-08-22</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>165</prism:startingPage>
		<prism:doi>10.3390/astronomy2030012</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/11">

	<title>Astronomy, Vol. 2, Pages 153-164: Simulation of Dynamic Evolution of Ring Current Ion Flux by a Lunar Base Energetic Neutral Atom (ENA) Imaging</title>
	<link>https://www.mdpi.com/2674-0346/2/3/11</link>
	<description>The distribution of energetic ion flux in the ring current region, such as a meteorological cumulonimbus cloud, stores up the particle energy for a geomagnetic substorm. It is helpful to study the geomagnetic substorm mechanism by using a lunar base ENA imaging simulation of the dynamic evolution of the ring current, and establishing the corresponding relationship between key node events of the substorm. Based on the previous observation experience and our simulation results of the dynamic evolution of the ring current, we propose a macroscopic model of substorms related to the dynamic evolution of ring currents and present the possibility of confirming the causal sequence of some of those critical node events of substorms with the lunar base ENA imaging measurement. IBEX, operating in the ecliptic plane, may even give examples of the telemetry of ring current ion fluxes through ENA measurements during substorms/quiets.</description>
	<pubDate>2023-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 153-164: Simulation of Dynamic Evolution of Ring Current Ion Flux by a Lunar Base Energetic Neutral Atom (ENA) Imaging</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/11">doi: 10.3390/astronomy2030011</a></p>
	<p>Authors:
		Li Lu
		Qinglong Yu
		Shuai Jia
		Zhong Xie
		Jian Lan
		Yuan Chang
		</p>
	<p>The distribution of energetic ion flux in the ring current region, such as a meteorological cumulonimbus cloud, stores up the particle energy for a geomagnetic substorm. It is helpful to study the geomagnetic substorm mechanism by using a lunar base ENA imaging simulation of the dynamic evolution of the ring current, and establishing the corresponding relationship between key node events of the substorm. Based on the previous observation experience and our simulation results of the dynamic evolution of the ring current, we propose a macroscopic model of substorms related to the dynamic evolution of ring currents and present the possibility of confirming the causal sequence of some of those critical node events of substorms with the lunar base ENA imaging measurement. IBEX, operating in the ecliptic plane, may even give examples of the telemetry of ring current ion fluxes through ENA measurements during substorms/quiets.</p>
	]]></content:encoded>

	<dc:title>Simulation of Dynamic Evolution of Ring Current Ion Flux by a Lunar Base Energetic Neutral Atom (ENA) Imaging</dc:title>
			<dc:creator>Li Lu</dc:creator>
			<dc:creator>Qinglong Yu</dc:creator>
			<dc:creator>Shuai Jia</dc:creator>
			<dc:creator>Zhong Xie</dc:creator>
			<dc:creator>Jian Lan</dc:creator>
			<dc:creator>Yuan Chang</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030011</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-08-22</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>153</prism:startingPage>
		<prism:doi>10.3390/astronomy2030011</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/3/10">

	<title>Astronomy, Vol. 2, Pages 141-152: Spins of Supermassive Black Holes M87* and SgrA* Revealed from the Size of Dark Spots in Event Horizon Telescope Images</title>
	<link>https://www.mdpi.com/2674-0346/2/3/10</link>
	<description>We reconstructed dark spots in the images of supermassive black holes SgrA* and M87* provided by the Event Horizon Telescope (EHT) collaboration by using the geometrically thin accretion disk model. In this model, the black hole is highlighted by the hot accretion matter up to the very vicinity of the black hole event horizon. The existence of hot accretion matter in the vicinity of black hole event horizons is predicted by the Blandford&amp;amp;ndash;Znajek mechanism, which is confirmed by recent general relativistic MHD simulations in supercomputers. A dark spot in the black hole image in the described model is a gravitationally lensed image of an event horizon globe. The lensed images of event horizons are always projected at the celestial sphere inside the awaited positions of the classical black hole shadows, which are invisible in both cases of M87* and SgrA*. We used the sizes of dark spots in the images of SgrA* and M87* for inferring their spins, 0.65&amp;amp;lt;a&amp;amp;lt;0.9 and a&amp;amp;gt;0.75, accordingly.</description>
	<pubDate>2023-07-19</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 141-152: Spins of Supermassive Black Holes M87* and SgrA* Revealed from the Size of Dark Spots in Event Horizon Telescope Images</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/3/10">doi: 10.3390/astronomy2030010</a></p>
	<p>Authors:
		Vyacheslav Ivanovich Dokuchaev
		</p>
	<p>We reconstructed dark spots in the images of supermassive black holes SgrA* and M87* provided by the Event Horizon Telescope (EHT) collaboration by using the geometrically thin accretion disk model. In this model, the black hole is highlighted by the hot accretion matter up to the very vicinity of the black hole event horizon. The existence of hot accretion matter in the vicinity of black hole event horizons is predicted by the Blandford&amp;amp;ndash;Znajek mechanism, which is confirmed by recent general relativistic MHD simulations in supercomputers. A dark spot in the black hole image in the described model is a gravitationally lensed image of an event horizon globe. The lensed images of event horizons are always projected at the celestial sphere inside the awaited positions of the classical black hole shadows, which are invisible in both cases of M87* and SgrA*. We used the sizes of dark spots in the images of SgrA* and M87* for inferring their spins, 0.65&amp;amp;lt;a&amp;amp;lt;0.9 and a&amp;amp;gt;0.75, accordingly.</p>
	]]></content:encoded>

	<dc:title>Spins of Supermassive Black Holes M87* and SgrA* Revealed from the Size of Dark Spots in Event Horizon Telescope Images</dc:title>
			<dc:creator>Vyacheslav Ivanovich Dokuchaev</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2030010</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-07-19</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-07-19</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>141</prism:startingPage>
		<prism:doi>10.3390/astronomy2030010</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/3/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/2/9">

	<title>Astronomy, Vol. 2, Pages 128-140: Lensing with Generalized Symmetrons</title>
	<link>https://www.mdpi.com/2674-0346/2/2/9</link>
	<description>Generalized symmetrons are models that have qualitatively similar features to the archetypal symmetron, but have barely been studied. In this article, we investigate for what parameter values the fifth forces induced by disformally coupling generalized symmetrons can provide an explanation for the difference between baryonic and lens masses of galaxies. While it is known that the standard symmetron struggles to provide an alternative source for the lensing otherwise attributed to particle dark matter, we show that some generalized symmetron models are more suitable for complying with existing constraints on disformal couplings. This motivates future studies of these only little-explored models.</description>
	<pubDate>2023-06-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 128-140: Lensing with Generalized Symmetrons</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/2/9">doi: 10.3390/astronomy2020009</a></p>
	<p>Authors:
		Christian Käding
		</p>
	<p>Generalized symmetrons are models that have qualitatively similar features to the archetypal symmetron, but have barely been studied. In this article, we investigate for what parameter values the fifth forces induced by disformally coupling generalized symmetrons can provide an explanation for the difference between baryonic and lens masses of galaxies. While it is known that the standard symmetron struggles to provide an alternative source for the lensing otherwise attributed to particle dark matter, we show that some generalized symmetron models are more suitable for complying with existing constraints on disformal couplings. This motivates future studies of these only little-explored models.</p>
	]]></content:encoded>

	<dc:title>Lensing with Generalized Symmetrons</dc:title>
			<dc:creator>Christian Käding</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2020009</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-06-07</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-06-07</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>128</prism:startingPage>
		<prism:doi>10.3390/astronomy2020009</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/2/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/2/8">

	<title>Astronomy, Vol. 2, Pages 105-127: Gravitational versus Magnetohydrodynamic Waves in Curved Spacetime in the Presence of Large-Scale Magnetic Fields</title>
	<link>https://www.mdpi.com/2674-0346/2/2/8</link>
	<description>The general-relativistic (GR) magnetohydrodynamic (MHD) equations for a conductive plasma fluid are derived and discussed in the curved spacetime described by Thorne&amp;amp;rsquo;s metric tensor, i.e., a family of cosmological models with inherent anisotropy due to the existence of an ambient, large-scale magnetic field. In this framework, it is examined whether the magnetized plasma fluid that drives the evolution of such a model can be subsequently excited by a transient, plane-polarized gravitational wave (GW) or not. To do so, we consider the associated set of the perturbed equations of motion and integrate them numerically in order to study the evolution of instabilities triggered by the GW propagation. In particular, we examine to what extend perturbations of the electric and/or the magnetic field can be amplified due to a potential energy transfer from the GW to the electromagnetic (EM) degrees of freedom. The evolution of the perturbed quantities depends on four free parameters, namely, the conductivity of the fluid, &amp;amp;sigma;; the speed of sound square, 13&amp;amp;lt;Csc2&amp;amp;equiv;&amp;amp;gamma;&amp;amp;lt;1, which in this model may serve also as a measure of the inherent anisotropy; the GW frequency, &amp;amp;omega;g; and the associated angle of propagation with respect to the direction of the magnetic field, &amp;amp;theta;. We find that GW propagation in the anisotropic magnetized medium under consideration does excite several MHD modes; in other words, there is energy transfer from the gravitational to the EM degrees of freedom that can result in the acceleration of charged particles at the spot and in the subsequent damping of the GW.</description>
	<pubDate>2023-06-01</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 105-127: Gravitational versus Magnetohydrodynamic Waves in Curved Spacetime in the Presence of Large-Scale Magnetic Fields</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/2/8">doi: 10.3390/astronomy2020008</a></p>
	<p>Authors:
		Kostas Kleidis
		Apostolos Kuiroukidis
		Demetrios B. Papadopoulos
		</p>
	<p>The general-relativistic (GR) magnetohydrodynamic (MHD) equations for a conductive plasma fluid are derived and discussed in the curved spacetime described by Thorne&amp;amp;rsquo;s metric tensor, i.e., a family of cosmological models with inherent anisotropy due to the existence of an ambient, large-scale magnetic field. In this framework, it is examined whether the magnetized plasma fluid that drives the evolution of such a model can be subsequently excited by a transient, plane-polarized gravitational wave (GW) or not. To do so, we consider the associated set of the perturbed equations of motion and integrate them numerically in order to study the evolution of instabilities triggered by the GW propagation. In particular, we examine to what extend perturbations of the electric and/or the magnetic field can be amplified due to a potential energy transfer from the GW to the electromagnetic (EM) degrees of freedom. The evolution of the perturbed quantities depends on four free parameters, namely, the conductivity of the fluid, &amp;amp;sigma;; the speed of sound square, 13&amp;amp;lt;Csc2&amp;amp;equiv;&amp;amp;gamma;&amp;amp;lt;1, which in this model may serve also as a measure of the inherent anisotropy; the GW frequency, &amp;amp;omega;g; and the associated angle of propagation with respect to the direction of the magnetic field, &amp;amp;theta;. We find that GW propagation in the anisotropic magnetized medium under consideration does excite several MHD modes; in other words, there is energy transfer from the gravitational to the EM degrees of freedom that can result in the acceleration of charged particles at the spot and in the subsequent damping of the GW.</p>
	]]></content:encoded>

	<dc:title>Gravitational versus Magnetohydrodynamic Waves in Curved Spacetime in the Presence of Large-Scale Magnetic Fields</dc:title>
			<dc:creator>Kostas Kleidis</dc:creator>
			<dc:creator>Apostolos Kuiroukidis</dc:creator>
			<dc:creator>Demetrios B. Papadopoulos</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2020008</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-06-01</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-06-01</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>105</prism:startingPage>
		<prism:doi>10.3390/astronomy2020008</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/2/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/2/7">

	<title>Astronomy, Vol. 2, Pages 90-104: The Quest for the Nature of the Dark Matter: The Need of a New Paradigm</title>
	<link>https://www.mdpi.com/2674-0346/2/2/7</link>
	<description>The phenomenon of the Dark matter baffles the researchers: the underlying dark particle has escaped so far the detection and its astrophysical role appears complex and entangled with that of the standard luminous particles. We propose that, in order to act efficiently, alongside with abandoning the current &amp;amp;Lambda;CDM scenario, we need also to shift the Paradigm from which it emerged.</description>
	<pubDate>2023-05-21</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 90-104: The Quest for the Nature of the Dark Matter: The Need of a New Paradigm</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/2/7">doi: 10.3390/astronomy2020007</a></p>
	<p>Authors:
		Fabrizio Nesti
		Paolo Salucci
		Nicola Turini
		</p>
	<p>The phenomenon of the Dark matter baffles the researchers: the underlying dark particle has escaped so far the detection and its astrophysical role appears complex and entangled with that of the standard luminous particles. We propose that, in order to act efficiently, alongside with abandoning the current &amp;amp;Lambda;CDM scenario, we need also to shift the Paradigm from which it emerged.</p>
	]]></content:encoded>

	<dc:title>The Quest for the Nature of the Dark Matter: The Need of a New Paradigm</dc:title>
			<dc:creator>Fabrizio Nesti</dc:creator>
			<dc:creator>Paolo Salucci</dc:creator>
			<dc:creator>Nicola Turini</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2020007</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-05-21</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-05-21</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>90</prism:startingPage>
		<prism:doi>10.3390/astronomy2020007</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/2/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/2/6">

	<title>Astronomy, Vol. 2, Pages 58-89: From a Dinuclear System to Close Binary Cosmic Objects</title>
	<link>https://www.mdpi.com/2674-0346/2/2/6</link>
	<description>Applying the ideas from microscopic objects to macroscopic stellar and galactic systems, the evolution of compact di-stars and di-galaxies is studied in the mass asymmetry coordinate. The formation of stable binary systems is analyzed. The role of symmetrization of an initially asymmetric binary system is revealed in the transformation of gravitational energy into internal energy of stars or galaxies accompanied by the release of a huge amount of energy. For the contact binary stars, the change of the orbital period is explained by evolution to symmetry in mass asymmetry coordinates. The matter transfer in binary black holes is studied. The conditions for the merger of black holes in a binary system are analyzed regarding the radiation of gravitational waves. Using the model based on the Regge-like laws, the Darwin instability effect in binary systems is discussed. New analytical formulas are derived for the period of orbital rotation and the relative distance between the components of a binary system. The impossibility of the appearance of a binary cosmic object from a single cosmic object is revealed.</description>
	<pubDate>2023-04-20</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 58-89: From a Dinuclear System to Close Binary Cosmic Objects</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/2/6">doi: 10.3390/astronomy2020006</a></p>
	<p>Authors:
		G. G. Adamian
		N. V. Antonenko
		H. Lenske
		V. V. Sargsyan
		</p>
	<p>Applying the ideas from microscopic objects to macroscopic stellar and galactic systems, the evolution of compact di-stars and di-galaxies is studied in the mass asymmetry coordinate. The formation of stable binary systems is analyzed. The role of symmetrization of an initially asymmetric binary system is revealed in the transformation of gravitational energy into internal energy of stars or galaxies accompanied by the release of a huge amount of energy. For the contact binary stars, the change of the orbital period is explained by evolution to symmetry in mass asymmetry coordinates. The matter transfer in binary black holes is studied. The conditions for the merger of black holes in a binary system are analyzed regarding the radiation of gravitational waves. Using the model based on the Regge-like laws, the Darwin instability effect in binary systems is discussed. New analytical formulas are derived for the period of orbital rotation and the relative distance between the components of a binary system. The impossibility of the appearance of a binary cosmic object from a single cosmic object is revealed.</p>
	]]></content:encoded>

	<dc:title>From a Dinuclear System to Close Binary Cosmic Objects</dc:title>
			<dc:creator>G. G. Adamian</dc:creator>
			<dc:creator>N. V. Antonenko</dc:creator>
			<dc:creator>H. Lenske</dc:creator>
			<dc:creator>V. V. Sargsyan</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2020006</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-04-20</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-04-20</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>58</prism:startingPage>
		<prism:doi>10.3390/astronomy2020006</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/2/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/1/5">

	<title>Astronomy, Vol. 2, Pages 47-57: Fitting Power Spectrum of Scalar Perturbations for Primordial Black Hole Production during Inflation</title>
	<link>https://www.mdpi.com/2674-0346/2/1/5</link>
	<description>A simple phenomenological fit for the power spectrum of scalar (curvature) perturbations during inflation is proposed to analytically describe slow roll of inflaton and formation of primordial black holes (PBH) in the early universe, in the framework of single-field models. The fit is given by a sum of the power spectrum of slow-roll inflation, needed for a viable description of the cosmic microwave background (CMB) radiation in agreement with Planck/BICEP/Keck measurements, and the log-normal (Gaussian) fit for the power spectrum enhancement (peak) needed for efficient PBH production, in the leading (model-independent) approximation. The T-type &amp;amp;alpha;-attractor models are used to get the simple CMB power spectrum depending upon the e-folds as the running variable. The location and height of the peak are chosen to yield the PBH masses in the asteroid-size window allowed for the whole (current) dark matter. We find the restrictions on the peak width.</description>
	<pubDate>2023-03-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 47-57: Fitting Power Spectrum of Scalar Perturbations for Primordial Black Hole Production during Inflation</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/1/5">doi: 10.3390/astronomy2010005</a></p>
	<p>Authors:
		Daniel Frolovsky
		Sergei V. Ketov
		</p>
	<p>A simple phenomenological fit for the power spectrum of scalar (curvature) perturbations during inflation is proposed to analytically describe slow roll of inflaton and formation of primordial black holes (PBH) in the early universe, in the framework of single-field models. The fit is given by a sum of the power spectrum of slow-roll inflation, needed for a viable description of the cosmic microwave background (CMB) radiation in agreement with Planck/BICEP/Keck measurements, and the log-normal (Gaussian) fit for the power spectrum enhancement (peak) needed for efficient PBH production, in the leading (model-independent) approximation. The T-type &amp;amp;alpha;-attractor models are used to get the simple CMB power spectrum depending upon the e-folds as the running variable. The location and height of the peak are chosen to yield the PBH masses in the asteroid-size window allowed for the whole (current) dark matter. We find the restrictions on the peak width.</p>
	]]></content:encoded>

	<dc:title>Fitting Power Spectrum of Scalar Perturbations for Primordial Black Hole Production during Inflation</dc:title>
			<dc:creator>Daniel Frolovsky</dc:creator>
			<dc:creator>Sergei V. Ketov</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2010005</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-03-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-03-22</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>47</prism:startingPage>
		<prism:doi>10.3390/astronomy2010005</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/1/4">

	<title>Astronomy, Vol. 2, Pages 22-46: On the Dynamical Instability of Monatomic Fluid Spheres in (N + 1)-Dimensional Spacetime</title>
	<link>https://www.mdpi.com/2674-0346/2/1/4</link>
	<description>In this note, I derive the Chandrasekhar instability of a fluid sphere in (N + 1)-dimensional Schwarzschild&amp;amp;ndash;Tangherlini spacetime and take the homogeneous (uniform energy density) solution for illustration. Qualitatively, the effect of a positive (negative) cosmological constant tends to destabilize (stabilize) the sphere. In the absence of a cosmological constant, the privileged position of (3 + 1)-dimensional spacetime is manifest in its own right. As it is, the marginal dimensionality in which a monatomic ideal fluid sphere is stable but not too stable to trigger the onset of gravitational collapse. Furthermore, it is the unique dimensionality that can accommodate stable hydrostatic equilibrium with a positive cosmological constant. However, given the current cosmological constant observed, no stable configuration can be larger than 1021M&amp;amp;#8857;. On the other hand, in (2 + 1) dimensions, it is too stable either in the context of Newtonian Gravity (NG) or Einstein&amp;amp;rsquo;s General Relativity (GR). In GR, the role of negative cosmological constant is crucial not only to guarantee fluid equilibrium (decreasing monotonicity of pressure) but also to have the Ba&amp;amp;ntilde;ados&amp;amp;ndash;Teitelboim&amp;amp;ndash;Zanelli (BTZ) black hole solution. Owing to the negativeness of the cosmological constant, there is no unstable configuration for a homogeneous fluid disk with mass 0&amp;amp;lt;M&amp;amp;le;0.5 to collapse into a naked singularity, which supports the Cosmic Censorship Conjecture. However, the relativistic instability can be triggered for a homogeneous disk with mass 0.5&amp;amp;lt;M&amp;amp;#8818;0.518 under causal limit, which implies that BTZ holes of mass MBTZ&amp;amp;gt;0 could emerge from collapsing fluid disks under proper conditions. The implicit assumptions and implications are also discussed.</description>
	<pubDate>2023-03-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 22-46: On the Dynamical Instability of Monatomic Fluid Spheres in (N + 1)-Dimensional Spacetime</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/1/4">doi: 10.3390/astronomy2010004</a></p>
	<p>Authors:
		Wei-Xiang Feng
		</p>
	<p>In this note, I derive the Chandrasekhar instability of a fluid sphere in (N + 1)-dimensional Schwarzschild&amp;amp;ndash;Tangherlini spacetime and take the homogeneous (uniform energy density) solution for illustration. Qualitatively, the effect of a positive (negative) cosmological constant tends to destabilize (stabilize) the sphere. In the absence of a cosmological constant, the privileged position of (3 + 1)-dimensional spacetime is manifest in its own right. As it is, the marginal dimensionality in which a monatomic ideal fluid sphere is stable but not too stable to trigger the onset of gravitational collapse. Furthermore, it is the unique dimensionality that can accommodate stable hydrostatic equilibrium with a positive cosmological constant. However, given the current cosmological constant observed, no stable configuration can be larger than 1021M&amp;amp;#8857;. On the other hand, in (2 + 1) dimensions, it is too stable either in the context of Newtonian Gravity (NG) or Einstein&amp;amp;rsquo;s General Relativity (GR). In GR, the role of negative cosmological constant is crucial not only to guarantee fluid equilibrium (decreasing monotonicity of pressure) but also to have the Ba&amp;amp;ntilde;ados&amp;amp;ndash;Teitelboim&amp;amp;ndash;Zanelli (BTZ) black hole solution. Owing to the negativeness of the cosmological constant, there is no unstable configuration for a homogeneous fluid disk with mass 0&amp;amp;lt;M&amp;amp;le;0.5 to collapse into a naked singularity, which supports the Cosmic Censorship Conjecture. However, the relativistic instability can be triggered for a homogeneous disk with mass 0.5&amp;amp;lt;M&amp;amp;#8818;0.518 under causal limit, which implies that BTZ holes of mass MBTZ&amp;amp;gt;0 could emerge from collapsing fluid disks under proper conditions. The implicit assumptions and implications are also discussed.</p>
	]]></content:encoded>

	<dc:title>On the Dynamical Instability of Monatomic Fluid Spheres in (N + 1)-Dimensional Spacetime</dc:title>
			<dc:creator>Wei-Xiang Feng</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2010004</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-03-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-03-02</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Technical Note</prism:section>
	<prism:startingPage>22</prism:startingPage>
		<prism:doi>10.3390/astronomy2010004</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/1/3">

	<title>Astronomy, Vol. 2, Pages 15-21: (No) Eternal Inflation in the Starobinsky Inflation Corrected by Higher Curvature Invariants</title>
	<link>https://www.mdpi.com/2674-0346/2/1/3</link>
	<description>The swampland criteria in string theory assert the no eternal inflation scenario. This work studied the impact of generic gravitational quantum corrections on eternal inflation. In particular, we find that the Starobinsky model of inflation should receive higher-order corrections stemming from quantum gravity. In this work, we studied the effect of the R3/2 and R4 corrections on the eternal inflation conditions for the Starobinsky model.</description>
	<pubDate>2023-02-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 15-21: (No) Eternal Inflation in the Starobinsky Inflation Corrected by Higher Curvature Invariants</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/1/3">doi: 10.3390/astronomy2010003</a></p>
	<p>Authors:
		Jan Chojnacki
		Jan Henryk Kwapisz
		</p>
	<p>The swampland criteria in string theory assert the no eternal inflation scenario. This work studied the impact of generic gravitational quantum corrections on eternal inflation. In particular, we find that the Starobinsky model of inflation should receive higher-order corrections stemming from quantum gravity. In this work, we studied the effect of the R3/2 and R4 corrections on the eternal inflation conditions for the Starobinsky model.</p>
	]]></content:encoded>

	<dc:title>(No) Eternal Inflation in the Starobinsky Inflation Corrected by Higher Curvature Invariants</dc:title>
			<dc:creator>Jan Chojnacki</dc:creator>
			<dc:creator>Jan Henryk Kwapisz</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2010003</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-02-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-02-22</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/astronomy2010003</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/1/2">

	<title>Astronomy, Vol. 2, Pages 14: Acknowledgment to the Reviewers of Astronomy in 2022</title>
	<link>https://www.mdpi.com/2674-0346/2/1/2</link>
	<description>High-quality academic publishing is built on rigorous peer review [...]</description>
	<pubDate>2023-01-16</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 14: Acknowledgment to the Reviewers of Astronomy in 2022</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/1/2">doi: 10.3390/astronomy2010002</a></p>
	<p>Authors:
		Astronomy Editorial Office Astronomy Editorial Office
		</p>
	<p>High-quality academic publishing is built on rigorous peer review [...]</p>
	]]></content:encoded>

	<dc:title>Acknowledgment to the Reviewers of Astronomy in 2022</dc:title>
			<dc:creator>Astronomy Editorial Office Astronomy Editorial Office</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2010002</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-01-16</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-01-16</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Editorial</prism:section>
	<prism:startingPage>14</prism:startingPage>
		<prism:doi>10.3390/astronomy2010002</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/2/1/1">

	<title>Astronomy, Vol. 2, Pages 1-13: Isoscalar Giant Monopole Resonance in Spherical Nuclei as a Nuclear Matter Incompressibility Indicator</title>
	<link>https://www.mdpi.com/2674-0346/2/1/1</link>
	<description>The incompressibility of both nuclear matter and finite nuclei is estimated by the monopole compression modes in nuclei in the framework of a nonrelativistic Hartree&amp;amp;ndash;Fock&amp;amp;ndash;Bogoliyubov method and the coherent density fluctuation model. The monopole states originate from vibrations of the nuclear density. The calculations in the model for the incompressibility in finite nuclei are based on the Brueckner energy&amp;amp;ndash;density functional for nuclear matter. Results for the energies of the breathing vibrational states and finite nuclei incompressibilities are obtained for various nuclei and their values are compared with recent experimental data. The evolution of the isoscalar giant monopole resonance (ISGMR) along Ni, Sn, and Pb isotopic chains is discussed. This approach can be applied to analyses of neutron stars properties, such as incompressibility, symmetry energy, slope parameter, and other astrophysical quantities, as well as for modelling dynamical behaviors within stellar environments.</description>
	<pubDate>2023-01-12</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 2, Pages 1-13: Isoscalar Giant Monopole Resonance in Spherical Nuclei as a Nuclear Matter Incompressibility Indicator</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/2/1/1">doi: 10.3390/astronomy2010001</a></p>
	<p>Authors:
		Mitko K. Gaidarov
		Martin V. Ivanov
		Yordan I. Katsarov
		Anton N. Antonov
		</p>
	<p>The incompressibility of both nuclear matter and finite nuclei is estimated by the monopole compression modes in nuclei in the framework of a nonrelativistic Hartree&amp;amp;ndash;Fock&amp;amp;ndash;Bogoliyubov method and the coherent density fluctuation model. The monopole states originate from vibrations of the nuclear density. The calculations in the model for the incompressibility in finite nuclei are based on the Brueckner energy&amp;amp;ndash;density functional for nuclear matter. Results for the energies of the breathing vibrational states and finite nuclei incompressibilities are obtained for various nuclei and their values are compared with recent experimental data. The evolution of the isoscalar giant monopole resonance (ISGMR) along Ni, Sn, and Pb isotopic chains is discussed. This approach can be applied to analyses of neutron stars properties, such as incompressibility, symmetry energy, slope parameter, and other astrophysical quantities, as well as for modelling dynamical behaviors within stellar environments.</p>
	]]></content:encoded>

	<dc:title>Isoscalar Giant Monopole Resonance in Spherical Nuclei as a Nuclear Matter Incompressibility Indicator</dc:title>
			<dc:creator>Mitko K. Gaidarov</dc:creator>
			<dc:creator>Martin V. Ivanov</dc:creator>
			<dc:creator>Yordan I. Katsarov</dc:creator>
			<dc:creator>Anton N. Antonov</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy2010001</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2023-01-12</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2023-01-12</prism:publicationDate>
	<prism:volume>2</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/astronomy2010001</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/2/1/1</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/16">

	<title>Astronomy, Vol. 1, Pages 271-287: Spin Optics for Gravitational Waves</title>
	<link>https://www.mdpi.com/2674-0346/1/3/16</link>
	<description>We present the geometric optics expansion for circularly polarized gravitational waves on a curved spacetime background, to subleading order. We call spin optics to the subleading order geometric optics expansion, which involves modifying the standard eikonal function by including a specially chosen helicity-dependent correction. We show that the techniques developed for the propagation of electromagnetic waves can also be applied to gravitational waves in the limit of spin optics. However, one needs to account for the difference in the photon and graviton helicity, which we do here.</description>
	<pubDate>2022-12-05</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 271-287: Spin Optics for Gravitational Waves</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/16">doi: 10.3390/astronomy1030016</a></p>
	<p>Authors:
		Pravin Kumar Dahal
		</p>
	<p>We present the geometric optics expansion for circularly polarized gravitational waves on a curved spacetime background, to subleading order. We call spin optics to the subleading order geometric optics expansion, which involves modifying the standard eikonal function by including a specially chosen helicity-dependent correction. We show that the techniques developed for the propagation of electromagnetic waves can also be applied to gravitational waves in the limit of spin optics. However, one needs to account for the difference in the photon and graviton helicity, which we do here.</p>
	]]></content:encoded>

	<dc:title>Spin Optics for Gravitational Waves</dc:title>
			<dc:creator>Pravin Kumar Dahal</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030016</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-12-05</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-12-05</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>271</prism:startingPage>
		<prism:doi>10.3390/astronomy1030016</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/16</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/15">

	<title>Astronomy, Vol. 1, Pages 255-270: Creating a CLOUDY-Compatible Database with CHIANTI Version 10 Data</title>
	<link>https://www.mdpi.com/2674-0346/1/3/15</link>
	<description>Atomic and molecular data are required to conduct the detailed calculations of microphysical processes performed by cloudy to predict the spectra of a theoretical model. cloudy now utilizes three atomic and molecular databases, one of which is CHIANTI version 7.1. CHIANTI version 10.0.1 is available, but its format has changed. cloudy is incompatible with the newer version. We have developed a script to convert the version 10.0.1 database into its version 7.1 format so that cloudy does not have to change every time there is a new CHIANTI version with an evolved format. This study outlines the steps taken by the script for this version format change. We have also found a modest number of significant changes to spectral line intensities/luminosities calculated by cloudy with the adoption of CHIANTI version 10.0.1. These changes are a result of improvements to collision strength data.</description>
	<pubDate>2022-11-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 255-270: Creating a CLOUDY-Compatible Database with CHIANTI Version 10 Data</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/15">doi: 10.3390/astronomy1030015</a></p>
	<p>Authors:
		Chamani M. Gunasekera
		Marios Chatzikos
		Gary J. Ferland
		</p>
	<p>Atomic and molecular data are required to conduct the detailed calculations of microphysical processes performed by cloudy to predict the spectra of a theoretical model. cloudy now utilizes three atomic and molecular databases, one of which is CHIANTI version 7.1. CHIANTI version 10.0.1 is available, but its format has changed. cloudy is incompatible with the newer version. We have developed a script to convert the version 10.0.1 database into its version 7.1 format so that cloudy does not have to change every time there is a new CHIANTI version with an evolved format. This study outlines the steps taken by the script for this version format change. We have also found a modest number of significant changes to spectral line intensities/luminosities calculated by cloudy with the adoption of CHIANTI version 10.0.1. These changes are a result of improvements to collision strength data.</p>
	]]></content:encoded>

	<dc:title>Creating a CLOUDY-Compatible Database with CHIANTI Version 10 Data</dc:title>
			<dc:creator>Chamani M. Gunasekera</dc:creator>
			<dc:creator>Marios Chatzikos</dc:creator>
			<dc:creator>Gary J. Ferland</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030015</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-11-28</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-11-28</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>255</prism:startingPage>
		<prism:doi>10.3390/astronomy1030015</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/15</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/14">

	<title>Astronomy, Vol. 1, Pages 246-254: Modified Gravity and a Space Probe&amp;ndash;Venus Mission</title>
	<link>https://www.mdpi.com/2674-0346/1/3/14</link>
	<description>A comparison of gravitational forces and a space probe&amp;amp;rsquo;s trajectory parameters is made for two different models of the sun&amp;amp;rsquo;s field, expressed in Schwarzschild and isotropic coordinates. It is shown that these two representations of a single Schwarzschild solution give, in the tangent space format, different deflections from classical finite trajectories and, hence, from one other; greatly amplified by a planet&amp;amp;rsquo;s (Venus&amp;amp;rsquo;) gravity assist, this effect renders it possible to experimentally specify the format of the gravity law that dominates the solar system.</description>
	<pubDate>2022-11-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 246-254: Modified Gravity and a Space Probe&amp;ndash;Venus Mission</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/14">doi: 10.3390/astronomy1030014</a></p>
	<p>Authors:
		Alexander P. Yefremov
		</p>
	<p>A comparison of gravitational forces and a space probe&amp;amp;rsquo;s trajectory parameters is made for two different models of the sun&amp;amp;rsquo;s field, expressed in Schwarzschild and isotropic coordinates. It is shown that these two representations of a single Schwarzschild solution give, in the tangent space format, different deflections from classical finite trajectories and, hence, from one other; greatly amplified by a planet&amp;amp;rsquo;s (Venus&amp;amp;rsquo;) gravity assist, this effect renders it possible to experimentally specify the format of the gravity law that dominates the solar system.</p>
	]]></content:encoded>

	<dc:title>Modified Gravity and a Space Probe&amp;amp;ndash;Venus Mission</dc:title>
			<dc:creator>Alexander P. Yefremov</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030014</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-11-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-11-18</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>246</prism:startingPage>
		<prism:doi>10.3390/astronomy1030014</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/14</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/13">

	<title>Astronomy, Vol. 1, Pages 235-245: Energetic Neutral Atom (ENA) Imaging Simulation of the Distant Planetary Magnetosphere and ENA Emission Discussion of the Solar Wind</title>
	<link>https://www.mdpi.com/2674-0346/1/3/13</link>
	<description>We doubt whether the &amp;amp;ldquo;Energetic Neutral Atom (ENA) ribbon&amp;amp;rdquo; signals, especially the peak ones, scanned remotely by IBEX-Hi at the lunar resonance orbit, are really from the heliopause, which involves assessing the scale of solar wind particle energy loss throughout the solar system. The ENA imaging simulation results at the Earth&amp;amp;rsquo;s orbit show that the scale of the planetary magnetosphere with a telemetry distance of AU magnitude is too small to contribute to the IBEX-Hi ribbon. However, the simulated effective ENA differential fluxes provide a reference for the physical scale evaluation of the huge magnetic structure in the heliopause. The ENA differential flux of the &amp;amp;ldquo;ENA emission cone&amp;amp;rdquo; generated by the charge exchange between the solar wind ion flow and local neutral gas near the Earth&amp;amp;rsquo;s orbit is also comparable to the measured peak of the IBEX-Hi ribbon, which may be the main ENA emission source of the ribbon&amp;amp;rsquo;s measured peak. The 2D ENA imaging measurements at the Lagrange points proposed here can be used to investigate the ENA ribbon origination by using the energy spectral lag vs the disparity of the ENA images.</description>
	<pubDate>2022-11-03</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 235-245: Energetic Neutral Atom (ENA) Imaging Simulation of the Distant Planetary Magnetosphere and ENA Emission Discussion of the Solar Wind</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/13">doi: 10.3390/astronomy1030013</a></p>
	<p>Authors:
		Li Lu
		Qinglong Yu
		Shuai Jia
		Yuan Chang
		</p>
	<p>We doubt whether the &amp;amp;ldquo;Energetic Neutral Atom (ENA) ribbon&amp;amp;rdquo; signals, especially the peak ones, scanned remotely by IBEX-Hi at the lunar resonance orbit, are really from the heliopause, which involves assessing the scale of solar wind particle energy loss throughout the solar system. The ENA imaging simulation results at the Earth&amp;amp;rsquo;s orbit show that the scale of the planetary magnetosphere with a telemetry distance of AU magnitude is too small to contribute to the IBEX-Hi ribbon. However, the simulated effective ENA differential fluxes provide a reference for the physical scale evaluation of the huge magnetic structure in the heliopause. The ENA differential flux of the &amp;amp;ldquo;ENA emission cone&amp;amp;rdquo; generated by the charge exchange between the solar wind ion flow and local neutral gas near the Earth&amp;amp;rsquo;s orbit is also comparable to the measured peak of the IBEX-Hi ribbon, which may be the main ENA emission source of the ribbon&amp;amp;rsquo;s measured peak. The 2D ENA imaging measurements at the Lagrange points proposed here can be used to investigate the ENA ribbon origination by using the energy spectral lag vs the disparity of the ENA images.</p>
	]]></content:encoded>

	<dc:title>Energetic Neutral Atom (ENA) Imaging Simulation of the Distant Planetary Magnetosphere and ENA Emission Discussion of the Solar Wind</dc:title>
			<dc:creator>Li Lu</dc:creator>
			<dc:creator>Qinglong Yu</dc:creator>
			<dc:creator>Shuai Jia</dc:creator>
			<dc:creator>Yuan Chang</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030013</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-11-03</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-11-03</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>235</prism:startingPage>
		<prism:doi>10.3390/astronomy1030013</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/13</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/12">

	<title>Astronomy, Vol. 1, Pages 222-234: Stability and Damping in the Disks of Massive Galaxies</title>
	<link>https://www.mdpi.com/2674-0346/1/3/12</link>
	<description>After their initial formation, disk galaxies are observed to be rotationally stable over periods of &amp;amp;gt;6 Gyr, implying that any large velocity disturbances of stars and gas clouds are damped rapidly on the timescale of their rotation. However, it is also known that despite this damping, there must be a degree of random local motion to stabilize the orbits against degenerate collapse. A mechanism for such damping is proposed by a combination of inter-stellar gravitational interactions, and interactions with the Oort clouds and exo-Oort objects associated with each star. These mechanisms may produce rapid damping of large perturbations within a time period that is short on the scale of observational look-back time, but long on the scale of the disk rotational period for stars with small perturbations. This mechanism may also account for the locally observed mean perturbations in the Milky Way of 8&amp;amp;ndash;15 km/s for younger stars and 20&amp;amp;ndash;30 km/s for older stars.</description>
	<pubDate>2022-10-14</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 222-234: Stability and Damping in the Disks of Massive Galaxies</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/12">doi: 10.3390/astronomy1030012</a></p>
	<p>Authors:
		John Herbert Marr
		</p>
	<p>After their initial formation, disk galaxies are observed to be rotationally stable over periods of &amp;amp;gt;6 Gyr, implying that any large velocity disturbances of stars and gas clouds are damped rapidly on the timescale of their rotation. However, it is also known that despite this damping, there must be a degree of random local motion to stabilize the orbits against degenerate collapse. A mechanism for such damping is proposed by a combination of inter-stellar gravitational interactions, and interactions with the Oort clouds and exo-Oort objects associated with each star. These mechanisms may produce rapid damping of large perturbations within a time period that is short on the scale of observational look-back time, but long on the scale of the disk rotational period for stars with small perturbations. This mechanism may also account for the locally observed mean perturbations in the Milky Way of 8&amp;amp;ndash;15 km/s for younger stars and 20&amp;amp;ndash;30 km/s for older stars.</p>
	]]></content:encoded>

	<dc:title>Stability and Damping in the Disks of Massive Galaxies</dc:title>
			<dc:creator>John Herbert Marr</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030012</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-10-14</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-10-14</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>222</prism:startingPage>
		<prism:doi>10.3390/astronomy1030012</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/12</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/3/11">

	<title>Astronomy, Vol. 1, Pages 126-221: K-Essence Lagrangians of Polytropic and Logotropic Unified Dark Matter and Dark Energy Models</title>
	<link>https://www.mdpi.com/2674-0346/1/3/11</link>
	<description>We determine the k-essence Lagrangian of a relativistic barotropic fluid. The equation of state of the fluid can be specified in different manners depending on whether the pressure is expressed in terms of the energy density (model I), the rest-mass density (model II), or the pseudo rest-mass density for a complex scalar field in the Thomas-Fermi approximation (model III). In the nonrelativistic limit, these three formulations coincide. In the relativistic regime, they lead to different models that we study exhaustively. We provide general results valid for an arbitrary equation of state and show how the different models are connected to each other. For illustration, we specifically consider polytropic and logotropic dark fluids that have been proposed as unified dark matter and dark energy models. We recover the Born-Infeld action of the Chaplygin gas in models I and III and obtain the explicit expression of the reduced action of the logotropic dark fluid in models II and III. We also derive the two-fluid representation of the Chaplygin and logotropic models. Our general formalism can be applied to many other situations such as Bose-Einstein condensates with a |&amp;amp;phi;|4 (or more general) self-interaction, dark matter superfluids, and mixed models.</description>
	<pubDate>2022-09-28</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 126-221: K-Essence Lagrangians of Polytropic and Logotropic Unified Dark Matter and Dark Energy Models</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/3/11">doi: 10.3390/astronomy1030011</a></p>
	<p>Authors:
		Pierre-Henri Chavanis
		</p>
	<p>We determine the k-essence Lagrangian of a relativistic barotropic fluid. The equation of state of the fluid can be specified in different manners depending on whether the pressure is expressed in terms of the energy density (model I), the rest-mass density (model II), or the pseudo rest-mass density for a complex scalar field in the Thomas-Fermi approximation (model III). In the nonrelativistic limit, these three formulations coincide. In the relativistic regime, they lead to different models that we study exhaustively. We provide general results valid for an arbitrary equation of state and show how the different models are connected to each other. For illustration, we specifically consider polytropic and logotropic dark fluids that have been proposed as unified dark matter and dark energy models. We recover the Born-Infeld action of the Chaplygin gas in models I and III and obtain the explicit expression of the reduced action of the logotropic dark fluid in models II and III. We also derive the two-fluid representation of the Chaplygin and logotropic models. Our general formalism can be applied to many other situations such as Bose-Einstein condensates with a |&amp;amp;phi;|4 (or more general) self-interaction, dark matter superfluids, and mixed models.</p>
	]]></content:encoded>

	<dc:title>K-Essence Lagrangians of Polytropic and Logotropic Unified Dark Matter and Dark Energy Models</dc:title>
			<dc:creator>Pierre-Henri Chavanis</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1030011</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-09-28</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-09-28</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>3</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>126</prism:startingPage>
		<prism:doi>10.3390/astronomy1030011</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/3/11</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/2/10">

	<title>Astronomy, Vol. 1, Pages 99-125: Some Remarks on Non-Singular Spherically Symmetric Space-Times</title>
	<link>https://www.mdpi.com/2674-0346/1/2/10</link>
	<description>A short review of spherically symmetric static regular black holes and spherically symmetric non-singular cosmological space-time is presented. Several models, including new ones, of regular black holes are considered. First, a large class of regular black holes having an inner de Sitter core with the related issue of a Cauchy horizon is investigated. Then, Black Bounce space-times, where the Cauchy horizon and therefore the related instabilities are absent, are discussed as valid alternatives to regular black holes with inner de Sitter cores. Friedman&amp;amp;ndash;Lema&amp;amp;icirc;tre&amp;amp;ndash;Robertson&amp;amp;ndash;Walker space-times admitting regular bounce solutions are also discussed. In the general analysis concerning the presence or absence of singularities in the equations of motion, the role of a theorem credited to Osgood is stressed.</description>
	<pubDate>2022-09-15</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 99-125: Some Remarks on Non-Singular Spherically Symmetric Space-Times</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/2/10">doi: 10.3390/astronomy1020010</a></p>
	<p>Authors:
		Lorenzo Sebastiani
		Sergio Zerbini
		</p>
	<p>A short review of spherically symmetric static regular black holes and spherically symmetric non-singular cosmological space-time is presented. Several models, including new ones, of regular black holes are considered. First, a large class of regular black holes having an inner de Sitter core with the related issue of a Cauchy horizon is investigated. Then, Black Bounce space-times, where the Cauchy horizon and therefore the related instabilities are absent, are discussed as valid alternatives to regular black holes with inner de Sitter cores. Friedman&amp;amp;ndash;Lema&amp;amp;icirc;tre&amp;amp;ndash;Robertson&amp;amp;ndash;Walker space-times admitting regular bounce solutions are also discussed. In the general analysis concerning the presence or absence of singularities in the equations of motion, the role of a theorem credited to Osgood is stressed.</p>
	]]></content:encoded>

	<dc:title>Some Remarks on Non-Singular Spherically Symmetric Space-Times</dc:title>
			<dc:creator>Lorenzo Sebastiani</dc:creator>
			<dc:creator>Sergio Zerbini</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1020010</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-09-15</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-09-15</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>99</prism:startingPage>
		<prism:doi>10.3390/astronomy1020010</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/2/10</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/2/9">

	<title>Astronomy, Vol. 1, Pages 93-98: Physical Origin of the Dark Spot in the First Image of Supermassive Black Hole SgrA*</title>
	<link>https://www.mdpi.com/2674-0346/1/2/9</link>
	<description>We elucidate the physical origin of the dark spot in the image of supermassive black hole SgrA* presented very recently by the EHT collaboration. It is argued that this dark spot, which is noticeably smaller than the classical black hole shadow, is the northern hemisphere of the event horizon globe. The classical black hole shadow is unseen in the image of SgrA*. The dark spot in the image of SgrA* is projected within the position of the classical black hole shadow on the celestial sphere. The outer boundary of this dark spot is an equator on the event horizon globe.</description>
	<pubDate>2022-08-22</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 93-98: Physical Origin of the Dark Spot in the First Image of Supermassive Black Hole SgrA*</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/2/9">doi: 10.3390/astronomy1020009</a></p>
	<p>Authors:
		Vyacheslav I. Dokuchaev
		</p>
	<p>We elucidate the physical origin of the dark spot in the image of supermassive black hole SgrA* presented very recently by the EHT collaboration. It is argued that this dark spot, which is noticeably smaller than the classical black hole shadow, is the northern hemisphere of the event horizon globe. The classical black hole shadow is unseen in the image of SgrA*. The dark spot in the image of SgrA* is projected within the position of the classical black hole shadow on the celestial sphere. The outer boundary of this dark spot is an equator on the event horizon globe.</p>
	]]></content:encoded>

	<dc:title>Physical Origin of the Dark Spot in the First Image of Supermassive Black Hole SgrA*</dc:title>
			<dc:creator>Vyacheslav I. Dokuchaev</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1020009</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-08-22</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-08-22</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>93</prism:startingPage>
		<prism:doi>10.3390/astronomy1020009</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/2/9</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/2/8">

	<title>Astronomy, Vol. 1, Pages 84-92: Rotating and Expanding Gas in Binary Post-AGB Stars</title>
	<link>https://www.mdpi.com/2674-0346/1/2/8</link>
	<description>There is a class of binary post-AGB stars (binary system including a post-AGB star) that are surrounded by Keplerian disks and outflows resulting from gas escaping from the disk. To date, there are seven sources that have been studied in detail through interferometric millimeter-wave maps of CO lines (ALMA/NOEMA). For the cases of the Red Rectangle, IW Carinae, IRAS 08544-4431, and AC Herculis, it is found that around &amp;amp;ge;85% of the total nebular mass is located in the disk with Keplerian dynamics. The remainder of the nebular mass is located in an expanding component. This outflow is probably a disk wind consisting of material escaping from the rotating disk. These sources are the disk-dominated nebulae. On the contrary, our maps and modeling of 89 Herculis, IRAS 19125+0343, and R Scuti, which allowed us to study their morphology, kinematics, and mass distribution, suggest that, in these sources, the outflow clearly is the dominant component of the nebula (&amp;amp;sim;75% of the total nebular mass), resulting in a new subclass of nebulae around binary post-AGB stars: the outflow-dominated sources.Besides CO, the chemistry of this type of source has been practically unknown thus far. We also present a very deep single-dish radio molecular survey in the 1.3, 2, 3, 7, and 13 mm bands (&amp;amp;sim;600 h of telescope time). Our results and detections allow us to classify our sources as O- or /C-rich. We also conclude that the calculated abundances of the detected molecular species other than CO are particularly low, compared with AGB stars. This fact is very significant in those sources where the rotating disk is the dominant component of the nebula.</description>
	<pubDate>2022-08-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 84-92: Rotating and Expanding Gas in Binary Post-AGB Stars</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/2/8">doi: 10.3390/astronomy1020008</a></p>
	<p>Authors:
		Iván Gallardo Cava
		Valentín Bujarrabal
		Javier Alcolea
		Miguel Gómez-Garrido
		Arancha Castro-Carrizo
		Hans Van Winckel
		Miguel Santander-García
		</p>
	<p>There is a class of binary post-AGB stars (binary system including a post-AGB star) that are surrounded by Keplerian disks and outflows resulting from gas escaping from the disk. To date, there are seven sources that have been studied in detail through interferometric millimeter-wave maps of CO lines (ALMA/NOEMA). For the cases of the Red Rectangle, IW Carinae, IRAS 08544-4431, and AC Herculis, it is found that around &amp;amp;ge;85% of the total nebular mass is located in the disk with Keplerian dynamics. The remainder of the nebular mass is located in an expanding component. This outflow is probably a disk wind consisting of material escaping from the rotating disk. These sources are the disk-dominated nebulae. On the contrary, our maps and modeling of 89 Herculis, IRAS 19125+0343, and R Scuti, which allowed us to study their morphology, kinematics, and mass distribution, suggest that, in these sources, the outflow clearly is the dominant component of the nebula (&amp;amp;sim;75% of the total nebular mass), resulting in a new subclass of nebulae around binary post-AGB stars: the outflow-dominated sources.Besides CO, the chemistry of this type of source has been practically unknown thus far. We also present a very deep single-dish radio molecular survey in the 1.3, 2, 3, 7, and 13 mm bands (&amp;amp;sim;600 h of telescope time). Our results and detections allow us to classify our sources as O- or /C-rich. We also conclude that the calculated abundances of the detected molecular species other than CO are particularly low, compared with AGB stars. This fact is very significant in those sources where the rotating disk is the dominant component of the nebula.</p>
	]]></content:encoded>

	<dc:title>Rotating and Expanding Gas in Binary Post-AGB Stars</dc:title>
			<dc:creator>Iván Gallardo Cava</dc:creator>
			<dc:creator>Valentín Bujarrabal</dc:creator>
			<dc:creator>Javier Alcolea</dc:creator>
			<dc:creator>Miguel Gómez-Garrido</dc:creator>
			<dc:creator>Arancha Castro-Carrizo</dc:creator>
			<dc:creator>Hans Van Winckel</dc:creator>
			<dc:creator>Miguel Santander-García</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1020008</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-08-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-08-02</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>84</prism:startingPage>
		<prism:doi>10.3390/astronomy1020008</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/2/8</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/2/7">

	<title>Astronomy, Vol. 1, Pages 58-83: Theoretical and Observational Constraints on Lunar Orbital Evolution in the Three-Body Earth-Moon-Sun System</title>
	<link>https://www.mdpi.com/2674-0346/1/2/7</link>
	<description>Extremely slow recession of the Moon from the Earth has been recently proposed and attributed to conversion of Earth&amp;amp;rsquo;s axial spin to lunar orbital momentum. This hypothesis is inconsistent with long-standing recognition that the Moon&amp;amp;rsquo;s orbit involves three-body interactions. This and other short-comings, such as Earth&amp;amp;rsquo;s spin loss being internal, are summarized here. Considering point-masses is justified by theory and observational data on other moons. We deduce that torque in the Earth-Moon-Sun system increases eccentricity of the lunar orbit but decreases its inclination over time. Consequently, the average lunar orbital radius is decreasing. We also show that lunar drift is too small to be constrained through lunar laser ranging measurements, mainly because atmospheric refraction corrections are comparatively large and variations in lunar cycles are under-sampled. Our findings support co-accretion and explain how orbits evolve in many-body point-mass systems.</description>
	<pubDate>2022-07-11</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 58-83: Theoretical and Observational Constraints on Lunar Orbital Evolution in the Three-Body Earth-Moon-Sun System</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/2/7">doi: 10.3390/astronomy1020007</a></p>
	<p>Authors:
		Anne M. Hofmeister
		Robert E. Criss
		Everett M. Criss
		</p>
	<p>Extremely slow recession of the Moon from the Earth has been recently proposed and attributed to conversion of Earth&amp;amp;rsquo;s axial spin to lunar orbital momentum. This hypothesis is inconsistent with long-standing recognition that the Moon&amp;amp;rsquo;s orbit involves three-body interactions. This and other short-comings, such as Earth&amp;amp;rsquo;s spin loss being internal, are summarized here. Considering point-masses is justified by theory and observational data on other moons. We deduce that torque in the Earth-Moon-Sun system increases eccentricity of the lunar orbit but decreases its inclination over time. Consequently, the average lunar orbital radius is decreasing. We also show that lunar drift is too small to be constrained through lunar laser ranging measurements, mainly because atmospheric refraction corrections are comparatively large and variations in lunar cycles are under-sampled. Our findings support co-accretion and explain how orbits evolve in many-body point-mass systems.</p>
	]]></content:encoded>

	<dc:title>Theoretical and Observational Constraints on Lunar Orbital Evolution in the Three-Body Earth-Moon-Sun System</dc:title>
			<dc:creator>Anne M. Hofmeister</dc:creator>
			<dc:creator>Robert E. Criss</dc:creator>
			<dc:creator>Everett M. Criss</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1020007</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-07-11</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-07-11</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>2</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>58</prism:startingPage>
		<prism:doi>10.3390/astronomy1020007</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/2/7</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/6">

	<title>Astronomy, Vol. 1, Pages 49-57: Surface Electromagnetic Waves near a Black Hole Event Horizon and Their Observational Consequences</title>
	<link>https://www.mdpi.com/2674-0346/1/1/6</link>
	<description>Localization phenomena in light, scattering from random fluctuations of matter fields and space&amp;amp;ndash;time metrics near a black hole horizon, were predicted to produce a pronounced peak in the angular distribution of second-harmonic light in the direction normal to the horizon. Therefore, the detection of second-harmonic generation may become a viable observational tool to study spacetime physics near event horizons of astronomical black holes. The light localization phenomena near the horizon may be facilitated by the existence of surface electromagnetic wave solutions. In this communication, we study such surface electromagnetic wave solutions near the horizon of a Schwarzschild metric, describing a black hole in vacuum. We demonstrate that such surface wave solutions must appear when quantum gravity effects are taken into account. Potential observational evidence of this effect is also discussed.</description>
	<pubDate>2022-06-07</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 49-57: Surface Electromagnetic Waves near a Black Hole Event Horizon and Their Observational Consequences</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/6">doi: 10.3390/astronomy1010006</a></p>
	<p>Authors:
		Igor I. Smolyaninov
		</p>
	<p>Localization phenomena in light, scattering from random fluctuations of matter fields and space&amp;amp;ndash;time metrics near a black hole horizon, were predicted to produce a pronounced peak in the angular distribution of second-harmonic light in the direction normal to the horizon. Therefore, the detection of second-harmonic generation may become a viable observational tool to study spacetime physics near event horizons of astronomical black holes. The light localization phenomena near the horizon may be facilitated by the existence of surface electromagnetic wave solutions. In this communication, we study such surface electromagnetic wave solutions near the horizon of a Schwarzschild metric, describing a black hole in vacuum. We demonstrate that such surface wave solutions must appear when quantum gravity effects are taken into account. Potential observational evidence of this effect is also discussed.</p>
	]]></content:encoded>

	<dc:title>Surface Electromagnetic Waves near a Black Hole Event Horizon and Their Observational Consequences</dc:title>
			<dc:creator>Igor I. Smolyaninov</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010006</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-06-07</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-06-07</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Communication</prism:section>
	<prism:startingPage>49</prism:startingPage>
		<prism:doi>10.3390/astronomy1010006</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/6</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/5">

	<title>Astronomy, Vol. 1, Pages 36-48: Exotic Cores with and without Dark-Matter Admixtures in Compact Stars</title>
	<link>https://www.mdpi.com/2674-0346/1/1/5</link>
	<description>We parameterize the core of compact spherical star configurations by a mass (mx) and a radius (rx) and study the resulting admissible areas in the total-mass&amp;amp;ndash;total-radius plane. The employed fiducial equation-of-state models of the corona at radii r&amp;amp;gt;rx and pressures p&amp;amp;le;px with p(r=rx)=px are that of constant sound velocity and a proxy of DY&amp;amp;Delta; DD-ME2 provided by Buchdahl&amp;amp;rsquo;s exactly solvable ansatz. The core (r&amp;amp;lt;rx) may contain any type of material, e.g., Standard-Model matter with unspecified equation of state or/and an unspecified Dark-Matter admixture. Employing a toy model for the cool equation of state with first-order phase transition, we also discuss the mass-radius relation of compact stars with an admixture of Dark Matter in a Mirror-World scenario.</description>
	<pubDate>2022-05-29</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 36-48: Exotic Cores with and without Dark-Matter Admixtures in Compact Stars</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/5">doi: 10.3390/astronomy1010005</a></p>
	<p>Authors:
		Rico Zöllner
		Burkhard Kämpfer
		</p>
	<p>We parameterize the core of compact spherical star configurations by a mass (mx) and a radius (rx) and study the resulting admissible areas in the total-mass&amp;amp;ndash;total-radius plane. The employed fiducial equation-of-state models of the corona at radii r&amp;amp;gt;rx and pressures p&amp;amp;le;px with p(r=rx)=px are that of constant sound velocity and a proxy of DY&amp;amp;Delta; DD-ME2 provided by Buchdahl&amp;amp;rsquo;s exactly solvable ansatz. The core (r&amp;amp;lt;rx) may contain any type of material, e.g., Standard-Model matter with unspecified equation of state or/and an unspecified Dark-Matter admixture. Employing a toy model for the cool equation of state with first-order phase transition, we also discuss the mass-radius relation of compact stars with an admixture of Dark Matter in a Mirror-World scenario.</p>
	]]></content:encoded>

	<dc:title>Exotic Cores with and without Dark-Matter Admixtures in Compact Stars</dc:title>
			<dc:creator>Rico Zöllner</dc:creator>
			<dc:creator>Burkhard Kämpfer</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010005</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-05-29</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-05-29</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>36</prism:startingPage>
		<prism:doi>10.3390/astronomy1010005</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/5</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/4">

	<title>Astronomy, Vol. 1, Pages 17-35: The Conformal Cosmological Potential</title>
	<link>https://www.mdpi.com/2674-0346/1/1/4</link>
	<description>We discuss qualitative features of the conformal relation between certain classes of gravity theories and general relativity, common to different themes such as f(R), Brans-Dicke-type, and string theories. We focus primarily on the frame relations of the fields involved, slice energy, traceless and Palatini extensions, and selected cosmological applications.</description>
	<pubDate>2022-04-02</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 17-35: The Conformal Cosmological Potential</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/4">doi: 10.3390/astronomy1010004</a></p>
	<p>Authors:
		Spiros Cotsakis
		Ifigeneia Klaoudatou
		Georgios Kolionis
		John Miritzis
		Dimitrios Trachilis
		</p>
	<p>We discuss qualitative features of the conformal relation between certain classes of gravity theories and general relativity, common to different themes such as f(R), Brans-Dicke-type, and string theories. We focus primarily on the frame relations of the fields involved, slice energy, traceless and Palatini extensions, and selected cosmological applications.</p>
	]]></content:encoded>

	<dc:title>The Conformal Cosmological Potential</dc:title>
			<dc:creator>Spiros Cotsakis</dc:creator>
			<dc:creator>Ifigeneia Klaoudatou</dc:creator>
			<dc:creator>Georgios Kolionis</dc:creator>
			<dc:creator>John Miritzis</dc:creator>
			<dc:creator>Dimitrios Trachilis</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010004</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-04-02</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-04-02</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Review</prism:section>
	<prism:startingPage>17</prism:startingPage>
		<prism:doi>10.3390/astronomy1010004</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/4</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/3">

	<title>Astronomy, Vol. 1, Pages 15-16: Astronomy&amp;mdash;Editorial</title>
	<link>https://www.mdpi.com/2674-0346/1/1/3</link>
	<description>Astronomy has a long history over thousands of years, since the creation of ancient civilization [...]</description>
	<pubDate>2022-03-18</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 15-16: Astronomy&amp;mdash;Editorial</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/3">doi: 10.3390/astronomy1010003</a></p>
	<p>Authors:
		Ignatios Antoniadis
		</p>
	<p>Astronomy has a long history over thousands of years, since the creation of ancient civilization [...]</p>
	]]></content:encoded>

	<dc:title>Astronomy&amp;amp;mdash;Editorial</dc:title>
			<dc:creator>Ignatios Antoniadis</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010003</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-03-18</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-03-18</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Editorial</prism:section>
	<prism:startingPage>15</prism:startingPage>
		<prism:doi>10.3390/astronomy1010003</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/3</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/2">

	<title>Astronomy, Vol. 1, Pages 2-14: 2+1 Einstein&amp;ndash;Klein&amp;ndash;Gordon Black Holes by Gravitational Decoupling</title>
	<link>https://www.mdpi.com/2674-0346/1/1/2</link>
	<description>In this work we study the 2+1-Einstein&amp;amp;ndash;Klein&amp;amp;ndash;Gordon system in the framework of Gravitational Decoupling. We associate the generic matter decoupling sector with a real scalar field so we can obtain a constraint which allows us to close the system of differential equations. The constraint corresponds to a differential equation involving the decoupling functions and the metric of the seed sector and will be independent of the scalar field itself. We show that when the equation admits analytical solutions, the scalar field and the self-interacting potential can be obtained straightforwardly. We found that, in the cases under consideration, it is possible to express the potential as an explicit function of the scalar field only for certain particular cases corresponding to limiting values of the parameters involved.</description>
	<pubDate>2022-02-24</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 2-14: 2+1 Einstein&amp;ndash;Klein&amp;ndash;Gordon Black Holes by Gravitational Decoupling</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/2">doi: 10.3390/astronomy1010002</a></p>
	<p>Authors:
		Pio J. Arias
		Pedro Bargueño
		Ernesto Contreras
		Ernesto Fuenmayor
		</p>
	<p>In this work we study the 2+1-Einstein&amp;amp;ndash;Klein&amp;amp;ndash;Gordon system in the framework of Gravitational Decoupling. We associate the generic matter decoupling sector with a real scalar field so we can obtain a constraint which allows us to close the system of differential equations. The constraint corresponds to a differential equation involving the decoupling functions and the metric of the seed sector and will be independent of the scalar field itself. We show that when the equation admits analytical solutions, the scalar field and the self-interacting potential can be obtained straightforwardly. We found that, in the cases under consideration, it is possible to express the potential as an explicit function of the scalar field only for certain particular cases corresponding to limiting values of the parameters involved.</p>
	]]></content:encoded>

	<dc:title>2+1 Einstein&amp;amp;ndash;Klein&amp;amp;ndash;Gordon Black Holes by Gravitational Decoupling</dc:title>
			<dc:creator>Pio J. Arias</dc:creator>
			<dc:creator>Pedro Bargueño</dc:creator>
			<dc:creator>Ernesto Contreras</dc:creator>
			<dc:creator>Ernesto Fuenmayor</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010002</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2022-02-24</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2022-02-24</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Article</prism:section>
	<prism:startingPage>2</prism:startingPage>
		<prism:doi>10.3390/astronomy1010002</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/2</prism:url>
	
	<cc:license rdf:resource="CC BY 4.0"/>
</item>
        <item rdf:about="https://www.mdpi.com/2674-0346/1/1/1">

	<title>Astronomy, Vol. 1, Pages 1: Publisher’s Note: Have You Ever Looked at the Stars?</title>
	<link>https://www.mdpi.com/2674-0346/1/1/1</link>
	<description>Have you ever looked at the stars [...]</description>
	<pubDate>2021-07-27</pubDate>

	<content:encoded><![CDATA[
	<p><b>Astronomy, Vol. 1, Pages 1: Publisher’s Note: Have You Ever Looked at the Stars?</b></p>
	<p>Astronomy <a href="https://www.mdpi.com/2674-0346/1/1/1">doi: 10.3390/astronomy1010001</a></p>
	<p>Authors:
		Yu Lin
		Ioana Craciun
		</p>
	<p>Have you ever looked at the stars [...]</p>
	]]></content:encoded>

	<dc:title>Publisher’s Note: Have You Ever Looked at the Stars?</dc:title>
			<dc:creator>Yu Lin</dc:creator>
			<dc:creator>Ioana Craciun</dc:creator>
		<dc:identifier>doi: 10.3390/astronomy1010001</dc:identifier>
	<dc:source>Astronomy</dc:source>
	<dc:date>2021-07-27</dc:date>

	<prism:publicationName>Astronomy</prism:publicationName>
	<prism:publicationDate>2021-07-27</prism:publicationDate>
	<prism:volume>1</prism:volume>
	<prism:number>1</prism:number>
	<prism:section>Editorial</prism:section>
	<prism:startingPage>1</prism:startingPage>
		<prism:doi>10.3390/astronomy1010001</prism:doi>
	<prism:url>https://www.mdpi.com/2674-0346/1/1/1</prism:url>
	
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