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Article

Tailoring Variations in the Microstructures, Linear/Nonlinear Optical, and Mechanical Properties of Dysprosium-Oxide-Reinforced Borate Glasses

by
Ahmed M. Henaish
1,2,*,
Osama M. Hemeda
1,
Enas A. Arrasheed
1,3,
Rizk M. Shalaby
4,
Ahmed R. Ghazy
1,
Ilya A. Weinstein
2,
Moustafa A. Darwish
1,
Ekaterina L. Trukhanova
5,*,
Alex V. Trukhanov
5,6,
Sergei V. Trukhanov
5,6,
Ahmed F. Al-Hossainy
7 and
Nermin A. Abdelhakim
4
1
Physics Department, Faculty of Science, Tanta University, Tanta 31527, Egypt
2
NANOTECH Center, Ural Federal University, 620002 Ekaterinburg, Russia
3
Department of Communication and Computer Engineering, Faculty of Engineering, Jadara University, Irbid 21110, Jordan
4
Metal Physics Laboratory Research, Department of Physics, Faculty of Science, Mansoura University, Mansoura 35516, Egypt
5
Laboratory of Magnetic Films Physics, SSPA “Scientific and Practical Materials Research Centre of NAS of Belarus”, 19, P. Brovki Str., 220072 Minsk, Belarus
6
Smart Sensor Systems Laboratory, Department of Electronic Materials Technology, National University of Science and Technology MISiS, 119049 Moscow, Russia
7
Chemistry Department, Faculty of Science, New Valley University, El-Kharga 72511, New Valley, Egypt
*
Authors to whom correspondence should be addressed.
J. Compos. Sci. 2023, 7(2), 61; https://doi.org/10.3390/jcs7020061
Submission received: 22 December 2022 / Revised: 12 January 2023 / Accepted: 1 February 2023 / Published: 6 February 2023
(This article belongs to the Section Composites Modelling and Characterization)
Browse Figures
Versions Notes

Abstract

:
Hybrid dysprosium-doped borate glassy samples [B-Gly/Dy]HDG (Borate Glass/Dysprosium)Hybrid Doped Glass were prepared in this study via the melt-quenching method. Its linear/nonlinear optical, photoluminescence, hardness indentation, and micro-creep properties were analyzed. The amorphous structure for all the prepared samples was confirmed from the XRD patterns. In addition, density functional theory (DFT), optimized by TD-DFT and Crystal Sleuth, was used to study the structure and crystallinity of the [B-Gly/Dy]HDG as isolated molecules and agreed with the peaks of experimental XRD patterns. Additionally, theoretical lattice types were studied using Polymorph, a content studio software, and orthorhombic Pc21b (29) and triclinic P-1 (2) structures were provided. Both mechanical and optical properties were responses to different concentrations of Dy2O3 in the glassy borate system. It was found that the length of indentation increases by increasing the load time, and the hardness decreases by increasing the load time. The stress exponent value also increased from 4.1 to 6.3. The indentation strain increases by increasing the load time. The direct optical band gap was evaluated using the Davis–Mott relation. Urbach energy and its connection to the disorder degree in materials were studied depending on the Dy2O3 concentration. The acquired optical parameters were also analyzed to determine the nonlinear refractive index as well as the linear and third-order nonlinear optical susceptibility of the investigated glass samples. The photoluminescence emission spectra were recorded, and their attributed transitions were studied. The mechanical studies showed that the hardness values increased by increasing Dy2O3 concentrations from 4160.54 to 5631.58 Mpa. The stress exponent value also increased from 4.1 to 6.3. Therefore, the higher value of stress exponent (S) is more resistant to indentation creep.

1. Introduction

With the diversity of glass compositions and improved analysis methods, glass structures suitable for every technological need have been created. Recently, a glass system based on borate reinforced with several oxides has been widely scrutinized due to its outstanding properties [1]. Boric oxide is used to make glass using BO3 units alone, and the BO3 units are converted to BO4 units by adding various cations. Due to the rupturing of B-O-B and the splitting of bridged oxygen [2,3,4,5,6]. Zinc oxide is often employed as a glass matrix modifier, causing defects by breaking the B-O-B link, forming non-bridged oxygen atoms, and creating dangling bonds [7,8,9,10,11,12]. Because of their unique properties, such as effective radiation shielding, a broad glass formation zone, and low melting temperatures, lead borate glasses are highly favored in technical applications [13,14]. Essentially, borate glass frameworks containing lead oxide are notable for their increased visual transmittance [15]. Over glass systems, the essential and optimum utilization of zinc and lead oxide as network exchangers decreases phonon energy [16,17]. Because of their ornamental qualities, rare earth elements are employed in glass production [18,19]. Because of the qualities of glass doped with rare earth elements, it may be used in various applications, including laser materials, plasma screens, optical waveguides, fiber amplifiers, and efficient amplifiers [20,21,22,23].
All oxide glasses based on (B2O3, SiO2, TeO2, and P4O6) have been proven to be the most suitable host materials for the progress of optoelectronic components [24,25]. It is possible to assume that glass based on borate is the most frequent variety because of its excellent transparency, chemical resistance, and thermal stability [26]. The low phonon energy host glass extends lower non-radiative relaxation rates and strong quantum efficiencies [27,28,29]. The optical homogeneity of the glassy matrix causes RE ions to display a variety of latent laser transitions. The spectroscopic analysis of RE ions in glasses yields information on the excited states’ transition probabilities, lifetimes, and branching ratios, all of which are important in the design and growth of different electro-optic and optical systems [30,31,32,33].
Neoteric TDDFT applications (DMol3 and Crystal Sleuth) for researching the structure of glass matrix, stability phase, and nanocomposite compounds [34,35,36] are reviewed. The use of this complete energy-based method for the estimation and investigation of spectroscopic properties has received little attention. This article discusses the structural study using a limited programming language [37]. The objective is to demonstrate that the same atomistic modeling techniques may be consistently employed throughout the experimental inquiry to achieve high levels of precision [38]. In order of crystallinity investigations, Polymorph used content studio software to study the possible crystal sites for the compounds and predict the final crystal structure of the system [39].
In the present work, the impact of Dy2O3 additive on the optical and mechanical characteristics of a novel glass system with chemical composition; (50 − x)B2O3 + 40Pb3O4 + 10CaO + xDy2O3 with the different substitution ratio of Dy2O3 (x = 0, 1, 2, 3, 4 and 5) was prepared. To explore and describe the modification of the bandgap structure, the UV–Vis absorbance spectra of the studied glass samples were investigated. The effect of adding different ratios of Dy2O3 on indentation creep behavior and micro-hardness values has been analyzed.

2. Materials and Methods

2.1. Materials and Reagents

All the oxides (raw materials) used in the study (B2O3, Pb3O4, CaO, and Dy2O3) were purchased from Oxford Laboratory. In contrast, dysprosium oxide was obtained from (Sigma-Aldrich, MO, USA) at a purity of 99.9%.

2.2. Experimental Procedure

The nominal compositions for the six studied glass samples (50 − x)B2O3 + 40Pb3O4 + 10CaO + xDy2O3 with varied Dy2O3 content (x = 0, 1, 2, 3, 4, and 5 wt%) were produced using the traditional solid-state approach. Dy0 (x = 0), Dy1 (x = 1), Dy2 (x = 2), Dy3 (x = 3), Dy4 (x = 4), and Dy5 (x = 5) were used to code the glass samples. Boron oxide (B2O3), lead oxide (Pb3O4), calcium oxide, and dysprosium oxide (Dy2O3) were well mixed before being pre-heated for 120 min at 300 degrees Celsius. The resulting formulations were thermally heated in a porcelain crucible at 1100 °C for 30 min before being cast onto a stainless-steel mold to originate glass samples in a disc form. The melting temperature of Dy2O3 increased from 1100 °C to 1300 °C when the substitution ratio of Dy2O3 increased. Following quenching, the produced samples were directly annealed in a muffle furnace set to 300 °C [34]. The structure of the samples has been studied at room temperature by powder X-ray diffraction analysis using a Bruker, AXS D8 Advance, Germany (Cu-Kα radiation). UV-visible absorption was recorded using the Shimadzu UV-2450 spectrophotometer at a range of (190–900 nm); all the measurements were taken at room temperature. Photoluminescence emission spectra were measured by HoRiBA (IHR 320) using a He-Cd laser with a wavelength of 442 nm as an excitation source.
A digital Vickers microhardness tester was used to accurately measure the hardness of glass specimens (Model FM-7 Future-Tech. Corp. Tokyo Japan). Micro indentation creep methods have substantial benefits in terms of speed, non-destructiveness, accuracy, and accessibility. For all types of glasses and surface treatments, only one indenter type may be utilized [35,36]. Although testing the softest and hardest materials under varying loads is more adaptive and accurate, the surface is subjected to standard stress for a record period using a pyramid-shaped diamond. An indentation is a pyramid with opposite sides that meet at a 136-degree angle. It applies 10 gf of diamond pressure to the material’s surface, and the impression size (typically no more than 0.5 mm) is assessed using a microscope. The Vickers indenter leaves an impression of a black square on a light background, swinging the microscope over a specimen to measure a ±1/1000 mm square depression. The area is calculated by averaging 10 measurements made across the diagonals for each sample.
The following formula is used to compute the number of Vickers (HV) [40,41]:
HV = 2 F   Sin ( 136 o / 2 ) / 2 / d 2  
meaning that HV = 1.854 F / d 2     approximately , where (F) and (d) are the applied load force and average diagonal length.

3. Results

3.1. Structural, Optical, and Mechanical Properties

3.1.1. X-ray Diffraction Analysis

The XRD spectral characteristics of the manufactured [B-Gly] and [B-Gly/Dy]HDG were compared with the characteristics of the system-isolated matrix (by TD-DFT simulation). The X-ray diffraction patterns of the manufactured glasses with various quantities of Dy2O3 additions are shown in Figure 1. This distinctive proved a completely amorphous nature for all samples under study. By changing the concentration of Dy2O3, the position and the intensity of the broad prominent peak at 2θ ≈ (29°) are changed.
The XRD patterns in Figure 2a,b demonstrate that [B-Gly] and [B-Gly/Dy5]HHG are nearly identical. The XRD analysis in Figure 2a,b indicates that [B-Gly] and [B-Gly/Dy5]HNC are almost similar at 2θ = 25.77°. For the different doped concentrations of dysprosium (lanthanides of inert transition elements), two peaks appeared at 2θ = 6.81° and 2θ = 13.62°. Table 1 demonstrates the relationship between the miller index (hkl) and the estimated average crystallite size (D), and the full width at half maximum (FWHM) absolute values. A good agreement between the interplanar distances (d) and the data in database code amcsd 96-411-7035 [42,43] and 0019483 [44] were observed. Diffraction peaks that were quite close to the [B-Gly] and [B-Gly/Dy]HDG measured data were generated by TDDFT and Crystal Sleuth Microsoft applications [45].
The X-ray diffraction pattern of [B-Gly] and [B-Gly/Dy]HDG was evaluated by applying the Debye–Scherrer relation, along with the Pesedo–Voigt function; the polarization nearly equal to 0.5 and 1 / d h k l = 0.0566 Å − 1 − 0.7446 Å − 1 , λ = 1.540562   Å , I 2 / I 1 = 0.5 in the range of 5 ≤ 2θ ≤ 80°. Using the formula of Scherer D = 0.9 λ / ( FWHM . cos θ ) , where λ = 1.541838 Å, which is the wavelength of the X-ray [46,47]. As presented in Table 1, features such as peak intensity, d-spacing (d), Miller indices (hkl), the average crystallite size (D), and FWHM were studied using the X-ray diffraction data from [B-Gly] and [B-Gly/Dy]HDG. The average crystalline size is ( D a v ) = 44.42   nm   and   150.32   nm for [B-Gly] and [B-Gly/Dy]HDG, respectively [48,49,50]. Additionally, theoretical X-ray diffraction models were determined by content studio software computations used in Polymorph [see (Figure 2 Inset)]. The integrals performed on the Brillouin zone are shown in the inset of Figure 2 with 2 x 2 x 1 (Polymorph [B-Gly] and [B-Gly/Dy]HDG. Estimated PXRD patterns were compared with the experimental XRD structures for the relevant experiment. There is only a slight difference in the position and strength of the specific peaks between the simulated and experimental XRD models; therefore, the general similarity has attracted much attention. Many factors influence the experimental XRD pattern, of which instrumentation and data collection techniques are only two [33].
The simulated XRD for [B-Gly]Iso and [B-Gly/Dy]Iso as isolated molecules provides orthorhombic Pc21b (29) and triclinic P-1 (2) structures, respectively. For the experimental patterns of [B-Gly] and [B-Gly/Dy]HDG, at 2θ equal to 25.77°, prominent peaks at hkl ( 020 ) appeared. Using the above assessment, the PXRD pattern accuracy of the fabricated material was validated. The atomic scale of [B-Gly]Iso and [B-Gly/Dy]Iso was estimated depending on the experimental and calculated PXRD patterns combination [51]. Additionally, the density of the defect was calculated by [52] δ = 1 D , specified as the dislocation line length per unit volume. The difference between average crystallite size calculation of borate glassy sample [B-Gly] and dysprosium doped borate glassy samples [B-Gly/Dy]HBG ( ∆ D A v ) by the equation of Scherrer and based on the highest peak of diffraction related to (020)1 crystal plane gives the value of ≅ ( ∆ D A v = 150.32 − 44.42 = 105.90   nm ). It can be conculcated that the high-value difference in crystallite size is an attribute to the high atomic mass of dysprosium (Mol. WtDy = 162.50), which is doped in the borate glassy samples [53].

3.1.2. UV–Vis Spectrum Analysis

The glass samples’ UV–Vis absorbance spectra were recorded at room temperature to define and describe the changes in the bandgap structure. The UV–Vis absorption spectra of all produced glass samples are shown in Figure 3.
The UV–Vis absorption spectra of the samples investigated demonstrate that the sample at x = 0 has a prominent UV absorption peak at around 432 nm. The glasses’ absorption band was expanded. Due to the amorphous nature of glass samples, there is no robust increase in absorption at energies near the band gap, which appears as an absorption edge in the UV–Vis absorption spectra. The broad band of near-visible light concentrated at around 425 nm shifted to a wider wavelength (redshift) of 435 nm, originating from band gap transitions with increasing Dy2O3 concentration levels. The absorbance spectrum shows an absorption band peak at 800 nm as Dy2O3 content was added to the glass: this peak is attributable to the spin-allowed transitions of Dy3+ at the ground state (6H15/2) into different exciting H states [49].
The Davis–Mott relation (2) has been utilized to generate optical energy gaps for the examined substances [54,55]:
α ( h v ) = x ( h v − E g ) 1 / n / h v  
where (Eg) denotes the optical energy band gap of the glass samples, (A) denotes a constant, (α) denotes the absorption coefficient, and hν denotes the incident spectrum photon energy. For direct transitions and plots of (αhν)2 vs. hν, calculated band gap energies for glass samples were studied using n = 2 and plots of (αhν)2 vs. hν, as shown in Figure 4. In the straight transition from 2.95 eV to 2.90 eV indicated in Table 2, the computed band gap energies were slightly adjusted from 3.07 eV for the sample at x = 0 to 3.09 eV at x = 5. As illustrated in Figure 3, the optical band gap reduces as the redshift in the absorption edge increases, resulting in a reduction in non-bridging oxygen (NBO). As a result, the glass structure is compressed [56,57].
In addition to the refractive index of glass samples, direct and indirect transitions were investigated using Equation (3) [58,59,60,61]:
n = ( 1 + R 1 − R ) + [ 4 R ( 1 − R ) 2 − K 2 ]   1 / 2  
where K (=αλ/4π) is the extinction coefficient, λ is the incident photons wavelength, and α is the absorption coefficient [62,63].
Table 2 shows the refractive index values in reverse order from the optical energy band gaps data. The refractive indices results show that the proposed glass system is a good candidate for photo-electronic and optical filter devices. The following formula describing the width of band tails was used to compute the Urbach energy (Eu), defined by [8,64,65].
L n ( α ) = L n ( α 0 ) + h ν / E u  
where (α) is the absorption coefficient, which is constant, and (Eu) is the Urbach energy.
(Eu) values have been extracted by plotting against and calculating the inverse of the slope for the curves that appear in Figure 5, giving Eu values. The values of the synthesized glass samples increased by increasing the Dy2O3 content, as shown in Table 2. The observed increase in Urbach’s energy in the range of 0.43–0.67 eV specifies the increase in the structural disorder of the glass samples [66].
The linear/nonlinear optical parameters were calculated; Figure 6a exhibits the studied glass samples’ refractive index variation versus the photon wavelength λ (nm). With the increasing wavelength, the refractive index decreases for all glass samples. The high refractive index below 380 nm is attributed to the effect of the main absorption. The refractive index is enhanced by increasing the Dy2O3 substitution in the glass system and reaches a minimum value at Dy2O3 content = 4 wt%. In general, this increase in the refractive index can be attributed to an increase in absorbance in the investigated samples, as given in Table 2 (1.5–1.49) and (0.89–4.13) for linear/nonlinear, respectively. The reflection increases for the fabricated glass samples due to the photons’ interaction on the samples with the filler compound ions and causing the photon to slow, and the refractive index also increases [67]. The value of the refractive index also increased with increases in the Dy2O3 content, owing to an increase in the atomic packing density by replacing the Dy element, which has a high relative atomic radius (162.5 pm), with a B element, which has a low relative atomic radius (84 pm). By adding the Dy2O3 to the glass lattice, the initial increase in the refractive is related to a change in the structural arrangements of the atoms in the glass matrix, which produces more non-bridging oxygen (NBO). NBOs are more polarizable than bridging oxygen (BO), which means increased polarizability of the glass through the increase in the NBOs produced due to Dy2O3 formation. Therefore, the invented samples are candidates used in photovoltaic and optical devices [6].
The extinction coefficient is distinctive and determines how strongly a form absorbs and reflects radiation or light at a certain wavelength [58]. Figure 6b shows the extinction coefficient spectra of all the glasses samples. When compared to the original glass, it can be seen that Dy2O3 incorporation caused increased absorption. This behavior is most likely related to the absorption spectra [68].
The nonlinear optical properties of glasses are significant and of enormous interest for photonic devices to be utilized in various technological applications with a wide spectrum of phenomena, such as optical solitons, optical frequency conversion, Raman dispersion, and phase conjugation. To understand the interaction of high-intensity light with matter, the nonlinear optical parameters, i.e., optical susceptibility χ(1), third-order optical susceptibility χ(3), and nonlinear refractive index n2, are very important. These parameters are estimated through a linear refractive index [69,70]. The increase or decrease in the nonlinear parameter and the optical band gap Eg may refer to the formation of BO bonds and ions of higher polarizability. It is enjoyable to note that n and n2 are usually immediately linked, such that high index (n and n2). Therefore, materials with a lower band gap seam exhibit an increased nonlinear optical behavior (sample x = 3). In general, in multi-component oxides, BO and NBO oxygens are in the glass matrix, which affected the value of χ3. These glass materials are promising for application as components of nonlinear optical devices.

3.2. Structural, Optical, and Mechanical Properties

Photoluminescence emission spectra of the investigated glass system at the excitation wavelength (425 nm = 2.92 eV) are shown in Figure 7a, and the values of λemission were shown. The value of E g p l (energy gap of photoluminescence) is between 2.15 and 2.23 since the emission peak is at an approximately constant wavelength value. It can show from the emission spectra of Dy0 that the prominent peak appears around (2.23 eV), and as doping by Dy2O3 appears, six emission bands peak at (1.46, 1.65, 1.86, 2.15, 2.40, and 2.54 eV) attributed to the transition from the (4F9/2 − 6H5/2, 4F9/2 − 6H9/2, 4F9/2 − 6H11/2, 4F9/2 − 6H13/2, 4F9/2 − 6H15/2 and 4I13/2 − 6H13/2), respectively [71,72]. A procedure for the deconvolution of the experimental spectra was required for more information and analysis of PL emission due to overlapping emission bands. All experimental curves were fitted by a superposition of several Gaussian components (R2 ≥ 0.998) using the standard numeric procedure, as shown in Figure 7b–f.

Hardness Indentation and Micro-Creep Dependence of Dy2O3 Composition

The resistance of a material ordered to indentation by a much harder body is known as the hardness of this material. It represents a measure of the resistance against lattice destruction or the resistance to permanent deformation or damage. Information about the strength, molecular bindings, yield strength, and elastic constants of the material is impeded by the hardness of the crystal. The plasticity of the crystal could be understood by a microhardness study of the crystal. In the hardness technique, the crystal is subjected to relatively high pressure on a limited area.
Figure 8 shows the creep behavior of six glass samples containing 0, 1, 2, 3, 4, and 5 wt% Dy2O3 concentrations, respectively, using the Vickers hardness test. The length of indentation increases by increasing the time for each sample [73]. Figure 9 shows the relationship between Vickers hardness and indentation time [74]. The irreversible plastic deformation of the material is represented by Vickers hardness, calculated from the residual projected area. The hardness decreases with increases in time in the interval from 5 s to 100 s, which is inverse relation to the length of indentation. The average hardness numbers of Dy0, Dy1, Dy2, Dy3, Dy4, and Dy5 are listed in Table 3. It is noted that average hardness values at t = 5 s rise by increasing Dy2O3 concentrations from 4160.54 to 5631.58 MPa. The stress exponent is computed from Equation (5) and listed in Table 2 according to [75,76]:
S = ⌊ ∂ ln d ˙ / ∂ lnH v ⌋ d  
The stress exponent studied using Equation (5) is used to define deformation mechanisms, where HV is the number of Vickers hardness, d is the length of indentation diagonal, and d ˙ is a variable rate of diagonal indentation length. The slope of a straight line obtained by plotting d ˙ against HV on the double logarithm scale is equal to the stress exponent (S), as shown in Figure 10 [77,78,79]. The stress exponent is an indication of the deformation mechanism at room temperature. The stress exponent (S) values range from 4.1 to 6.3, as shown in Table 2. Grain boundary sliding is related to n ≈ 2, and the dislocation movement, such as a creep, is related to n ≈ (5–7).
The indentation creep behavior is shown in Figure 11 by plotting strain against indentation time (indentation creep curve) of all glass samples [80]. The first stage shows a faster increase in strain with indentation time, starting from the beginning to 10 sec of indentation time [81,82,83]. The second stage indicates a slow-increasing region for all glass samples where the strain has a slow increase. No specimen breakage occurs because the hardness test is a compression test [84,85,86]. Therefore, the third stage cannot be recorded as it did in an ordinary creep test. Thus, the higher stress exponent (S) value is more resistant to the indentation creep [87,88,89].

4. Conclusions

The effects of dysprosium oxide being added to the glass system with the chemical composition (50 − x)B2O3 + 40Pb3O4 + 10CaO + xDy2O3, along with different substitution ratios on the structure, optical and mechanical properties, were investigated. All studied glasses were prepared using the melt-quenching technique. XRD analysis confirms the amorphous phase of the samples. Theoretical structural studies agreed with the XRD experimental data and predicted the formation of orthorhombic Pc21b (29) and triclinic P-1 (2) structures for the isolated molecules. The UV–VIS spectra were also recorded to evaluate important optical properties such as direct and indirect optical band gap, Urbach energy, and refractive index. It was observed that it varied between 2.93 and 4.06 at a wavelength of 700 nm. The indirect energy gap fluctuated around 2.95 eV, and the direct value of the energy gap was decreased by increasing Dy2O3 to reach a maximum (3.14 eV) at x = 1.
In contrast, other essential properties such as χ3, χ1, and n2 enhanced with an increase in Dy2O3 concentration, which could be useful for optoelectronics and solar cell application. The mechanical studies showed that the hardness values increased by increasing Dy2O3 concentrations from 4160.54 to 5631.58 Mpa. The stress exponent value also increased from 4.1 to 6.3. Therefore, the higher value of stress exponent (S) is more resistant to the indentation creep.

Author Contributions

Conceptualization, A.M.H., E.A.A., R.M.S., A.R.G., I.A.W., A.V.T., S.V.T. and A.F.A.-H.; methodology, A.M.H., A.R.G., I.A.W., M.A.D. and A.F.A.-H.; software, M.A.D., and E.L.T.; validation, O.M.H., M.A.D. and E.L.T.; formal analysis, A.M.H., E.A.A., R.M.S., A.R.G. and E.L.T.; investigation, A.M.H., E.A.A., R.M.S., A.R.G., A.V.T., S.V.T. and N.A.A.; resources, M.A.D., A.V.T. and S.V.T.; data curation, M.A.D., A.V.T. and S.V.T.; writing—original draft preparation, O.M.H., E.A.A., R.M.S., I.A.W., A.V.T., S.V.T., A.F.A.-H. and N.A.A.; writing—review and editing, A.M.H., O.M.H., A.R.G., I.A.W., A.V.T., S.V.T., A.F.A.-H. and N.A.A.; visualization, M.A.D. and E.L.T.; supervision, O.M.H., A.V.T., S.V.T. and A.F.A.-H.; project administration, A.V.T. and S.V.T.; funding acquisition, E.L.T., A.V.T. and S.V.T. All authors have read and agreed to the published version of the manuscript.

Funding

I.A.W. thanks the Ministry of Science and Higher Education of Russia, research project no. FEUZ-2023-0014 for support.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. XRD diffractogram for [B-Gly] with different concentrations of Dy2O3 glass system.
Figure 1. XRD diffractogram for [B-Gly] with different concentrations of Dy2O3 glass system.
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Figure 2. (a) PXRD patterns (combined experimental and simulated) for [B-Gly] and [B-Gly]Iso isolate molecule. Insert is a 3D orthorhombic Pc21b (29) lattice-type computed using the Polymorph method. (b) [B-Gly/Dy]HDG and [B-Gly/Dy]Iso isolate molecule. Inset is a 3D Monoclinic P-1(2) lattice type.
Figure 2. (a) PXRD patterns (combined experimental and simulated) for [B-Gly] and [B-Gly]Iso isolate molecule. Insert is a 3D orthorhombic Pc21b (29) lattice-type computed using the Polymorph method. (b) [B-Gly/Dy]HDG and [B-Gly/Dy]Iso isolate molecule. Inset is a 3D Monoclinic P-1(2) lattice type.
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Figure 3. UV–Vis absorption spectrum of the prepared glass samples; the inset figure shows the optical band gap as a function of Dy2O3 content.
Figure 3. UV–Vis absorption spectrum of the prepared glass samples; the inset figure shows the optical band gap as a function of Dy2O3 content.
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Figure 4. The dependence of (αhν)2 on the photon energy (hν) for the prepared glass samples.
Figure 4. The dependence of (αhν)2 on the photon energy (hν) for the prepared glass samples.
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Figure 5. The plot of ln(α) with hν of glass samples; inset shows the Eu as a function of Dy2O3 content.
Figure 5. The plot of ln(α) with hν of glass samples; inset shows the Eu as a function of Dy2O3 content.
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Figure 6. The relationship between the investigated glass samples (a) refractive index (n) and (b) extinction coefficient (K) for different concentrations of Dy2O3 on the wavelength λ (nm).
Figure 6. The relationship between the investigated glass samples (a) refractive index (n) and (b) extinction coefficient (K) for different concentrations of Dy2O3 on the wavelength λ (nm).
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Figure 7. Photoluminescence and deconvolution of photoluminescence spectra for different concentrations of Dy2O3 on the wavelength λ (530 nm).
Figure 7. Photoluminescence and deconvolution of photoluminescence spectra for different concentrations of Dy2O3 on the wavelength λ (530 nm).
Jcs 07 00061 g007aJcs 07 00061 g007b
Jcs 07 00061 g008 550
Figure 8. Variation of indentation length with time at constant load 100 gf.
Figure 8. Variation of indentation length with time at constant load 100 gf.
Jcs 07 00061 g008
Jcs 07 00061 g009 550
Figure 9. Variation of hardness with time at constant load 100 gf.
Figure 9. Variation of hardness with time at constant load 100 gf.
Jcs 07 00061 g009
Jcs 07 00061 g010 550
Figure 10. ln-ln of the Vickers hardness numbers against the dwell time of indentation at load 100 gf.
Figure 10. ln-ln of the Vickers hardness numbers against the dwell time of indentation at load 100 gf.
Jcs 07 00061 g010
Jcs 07 00061 g011 550
Figure 11. The creep behavior of different concentrations of Dy2O3 glass system.
Figure 11. The creep behavior of different concentrations of Dy2O3 glass system.
Jcs 07 00061 g011
Table
Table 1. The experimental and calculated XRD data using the Refine Version 3.0 (Carnegie Mellon University, Pennsylvania) Software Program (Kurt Barthelme’s & Bob Downs) for experimental [B-Gly] and [B-Gly/Dy]HDG and simulated parts [B-Gly]Iso and [B-Gly/Dy]Iso.
Table 1. The experimental and calculated XRD data using the Refine Version 3.0 (Carnegie Mellon University, Pennsylvania) Software Program (Kurt Barthelme’s & Bob Downs) for experimental [B-Gly] and [B-Gly/Dy]HDG and simulated parts [B-Gly]Iso and [B-Gly/Dy]Iso.
SymmetryObservedComputed
2θ (°)d (Å)hklFWHMInt. (a)2θ (°)d (Å) D A v δ     ( d )
[B-Gly] Orthorhombic Pc21b (29)
a = 7.74; b = 9.06 and c = 14.82Å25.773.4540205.19451316.8726.163.4569.159109.2
α = γ = β = 90°; V = 1153(4);35.632.554 4 ¯ 21 0.5971192.57135.552.56179.6812.55
rmse (b)= 0.00002625, Average 2.8958 44.4260.87
[B-Gly/Dy]HDG Monoclinic2 C1c1(9)6.77114.1531012.4289690.4936.80814.069195.8851.05
a = 6.88; b = 6.89; c = 6.9312.3437.48592014.05951067.4112.697.2745117.2085.32
α = 90.0; β = 110(1)°, γ = 90.0°25.0713.62460205.86254650.1124.983.637381.160123.2
Machine error = 0.53131.1802.9146 5 ¯ 144.47352020.2331.352.8985106.3594.03
V = 1600(37); 34.1012.6674 6 ¯ 050.597192.039033.932.681079.680125.5
rmse (b) = 0.0012335.6322.5545 4 ¯ 210.222840.713035.552.5605213.5446.83
38.4172.3728 4 ¯ 245.229193.83538.582.363290.990109.9
45.7982.0016 1 ¯ 322.7222140.68145.702.0057174.7857.22
58.3291.5939 7 ¯ 311.793189.251058.371.5928265.3437.69
62.2041.5027 1 ¯ 112.2945116.48462.191.5029207.3648.23
Average 150.3277.90
Intensity: (b) root-mean-square error; (b) nm and (c) = 10−3. (a)—lattice parameters, and (d)—Crystallite size.
Table
Table 2. Concentration (C), Urbach energy (Eu), energy gap indirect (EOIn), energy gap direct (EOD), linear refractive index (n), ( χ 1 ,   χ 3 ) linear and third-order nonlinear optical susceptibility for the prepared glass samples.
Table 2. Concentration (C), Urbach energy (Eu), energy gap indirect (EOIn), energy gap direct (EOD), linear refractive index (n), ( χ 1 ,   χ 3 ) linear and third-order nonlinear optical susceptibility for the prepared glass samples.
SamplesC (wt%)Eu (eV)EOD (eV)λcut-off (nm)n(a)χ1χ3 (b)n2 (c)
1X = 00.433.074321.350.0663.190.89
2X = 10.523.144261.380.0724.631.26
3X = 20.563.114291.390.0734.881.32
4X = 30.573.054381.550.1120.266.5
5X = 40.553.074331.370.0714.311.18
6X = 50.673.094351.490.0990.164.13
(a) = (linear refractive index); (b) = 10−15, (c) = (non-linear refractive index) 10−15 at (λ = 700 nm).
Table
Table 3. Hardness and stress exponent value at 5 sec and load 100 gf.
Table 3. Hardness and stress exponent value at 5 sec and load 100 gf.
SampleC (wt%)HV (MPa)S
1x = 04160.544.2
2x = 13835.404.1
3x = 24616.065.5
4x = 35103.685.9
5x = 45223.205.6
6x = 55631.586.3
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Henaish, A.M.; Hemeda, O.M.; Arrasheed, E.A.; Shalaby, R.M.; Ghazy, A.R.; Weinstein, I.A.; Darwish, M.A.; Trukhanova, E.L.; Trukhanov, A.V.; Trukhanov, S.V.; et al. Tailoring Variations in the Microstructures, Linear/Nonlinear Optical, and Mechanical Properties of Dysprosium-Oxide-Reinforced Borate Glasses. J. Compos. Sci. 2023, 7, 61. https://doi.org/10.3390/jcs7020061

AMA Style

Henaish AM, Hemeda OM, Arrasheed EA, Shalaby RM, Ghazy AR, Weinstein IA, Darwish MA, Trukhanova EL, Trukhanov AV, Trukhanov SV, et al. Tailoring Variations in the Microstructures, Linear/Nonlinear Optical, and Mechanical Properties of Dysprosium-Oxide-Reinforced Borate Glasses. Journal of Composites Science. 2023; 7(2):61. https://doi.org/10.3390/jcs7020061

Chicago/Turabian Style

Henaish, Ahmed M., Osama M. Hemeda, Enas A. Arrasheed, Rizk M. Shalaby, Ahmed R. Ghazy, Ilya A. Weinstein, Moustafa A. Darwish, Ekaterina L. Trukhanova, Alex V. Trukhanov, Sergei V. Trukhanov, and et al. 2023. "Tailoring Variations in the Microstructures, Linear/Nonlinear Optical, and Mechanical Properties of Dysprosium-Oxide-Reinforced Borate Glasses" Journal of Composites Science 7, no. 2: 61. https://doi.org/10.3390/jcs7020061

APA Style

Henaish, A. M., Hemeda, O. M., Arrasheed, E. A., Shalaby, R. M., Ghazy, A. R., Weinstein, I. A., Darwish, M. A., Trukhanova, E. L., Trukhanov, A. V., Trukhanov, S. V., Al-Hossainy, A. F., & Abdelhakim, N. A. (2023). Tailoring Variations in the Microstructures, Linear/Nonlinear Optical, and Mechanical Properties of Dysprosium-Oxide-Reinforced Borate Glasses. Journal of Composites Science, 7(2), 61. https://doi.org/10.3390/jcs7020061

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