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Quantum Nonstationary Systems

A special issue of Entropy (ISSN 1099-4300). This special issue belongs to the section "Quantum Information".

Deadline for manuscript submissions: closed (30 June 2023) | Viewed by 18627

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Instituto de Física e Centro Internacional de Física, Universidade de Brasília, Caixa Postal 04455, Brasília 70910-900, DF, Brazil
Interests: quantum physics; cavity electrodynamics; quantum closed and open systems with time-dependent parameters; uncertainty relations in quantum mechanics; nonclassical states of light in quantum optics
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Special Issue Information

Dear Colleagues,

Although time-dependent quantum systems have been studied since the very beginning of quantum mechanics, they continue to attract the attention of researchers, and almost every decade new important discoveries or new fields of application were made. Among the impressive results or by-products of these studies, one should note the discovery of the path integral method in the 1940s, coherent and squeezed states in the 1960–70s, quantum tunnelling in Josephson contacts and SQUIDs in the 1960s, the theory of time-dependent quantum invariants in the 1960–70s, different forms of quantum master equations in the 1960–70s, the Zeno effect in the 1970s, the concept of geometric phase in the 1980s, decoherence of macroscopic superpositions in the 1980s, quantum non-demolition measurements in the 1980s, dynamics of particles in quantum traps and cavity QED in the 1980–90s, and time-dependent processes in mesoscopic quantum devices in the 1990s. All these topics continue to be the subject of many publications.

Now we are witnessing a new wave of interest in quantum non-stationary systems in different areas, from cosmology (the very first moments of the Universe) and quantum field theory (particle pair creation in ultra-strong fields) to elementary particle physics (neutrino oscillations). A rapid increase in the number of theoretical and experimental works on time-dependent phenomena is also observed in quantum optics, quantum information theory and condensed matter physics. Time-dependent tunnelling and time-dependent transport in nano-structures are examples of such phenomena. Another emerging direction of study, stimulated by impressive progress in experimental techniques, is related to attempts to observe the quantum behavior of macroscopic objects, such as mirrors interacting with quantum fields in nano-resonators. Quantum effects manifest themselves in the dynamics of nano-electromechanical systems; they are dominant in the new field of circuit QED. Another rapidly growing research field is the quantum control of evolution at the microscopic level. These examples show that quantum non-stationary systems continue to be a living and very interesting part of quantum physics.

We invite researchers interested in the areas described above to submit contributions to this Special Issue. Topics of primary interest include (but are not limited to):

  • dynamics of quantum systems in the presence of dissipation;
  • dynamics of decoherence;
  • dynamics of quantum entanglement;
  • dynamics of optomechanical systems;
  • dynamical Casimir effect and its analogs;
  • dynamics of wave packets;
  • time-dependent scattering and tunnelling;
  • quantum speed limits and energy-time uncertainty relations;
  • quantum effects in nonstationary environments;
  • quantum invariants in systems with time-dependent parameters;
  • exact and approximate solutions in quantum mechanics with time-dependent parameters

Prof. Dr. Viktor Dodonov
Guest Editor

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Published Papers (10 papers)

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Research

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17 pages, 8787 KiB  
Article
Multipole Approach to the Dynamical Casimir Effect with Finite-Size Scatterers
by Lucas Alonso, Guilherme C. Matos, François Impens, Paulo A. Maia Neto and Reinaldo de Melo e Souza
Entropy 2024, 26(3), 251; https://doi.org/10.3390/e26030251 - 12 Mar 2024
Cited by 1 | Viewed by 1176
Abstract
A mirror subjected to a fast mechanical oscillation emits photons out of the quantum vacuum—a phenomenon known as the dynamical Casimir effect (DCE). The mirror is usually treated as an infinite metallic surface. Here, we show that, in realistic experimental conditions (mirror size [...] Read more.
A mirror subjected to a fast mechanical oscillation emits photons out of the quantum vacuum—a phenomenon known as the dynamical Casimir effect (DCE). The mirror is usually treated as an infinite metallic surface. Here, we show that, in realistic experimental conditions (mirror size and oscillation frequency), this assumption is inadequate and drastically overestimates the DCE radiation. Taking the opposite limit, we use instead the dipolar approximation to obtain a simpler and more realistic treatment of DCE for macroscopic bodies. Our approach is inspired by a microscopic theory of DCE, which is extended to the macroscopic realm by a suitable effective Hamiltonian description of moving anisotropic scatterers. We illustrate the benefits of our approach by considering the DCE from macroscopic bodies of different geometries. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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21 pages, 877 KiB  
Article
Partial Bell-State Measurement with Type-II Parametric Down Conversion: Extracting Phase Information from the Zeropoint Field (I)
by Alberto Casado and Santiago Guerra
Entropy 2023, 25(3), 393; https://doi.org/10.3390/e25030393 - 21 Feb 2023
Cited by 1 | Viewed by 1816
Abstract
In this paper, the nexus between the Bell-state measurement and extracting phase information from the zeropoint field is investigated. For this purpose, the Wigner representation in the Heisenberg picture is applied in a Bell-type experiment in which the polarisation-entangled photon pairs generated in [...] Read more.
In this paper, the nexus between the Bell-state measurement and extracting phase information from the zeropoint field is investigated. For this purpose, the Wigner representation in the Heisenberg picture is applied in a Bell-type experiment in which the polarisation-entangled photon pairs generated in a type-II parametric down-conversion do not overlap. The signal intensities at the detectors are calculated in a four-mode approximation, being expressed as functions of the modules and phases of the four zeropoint amplitudes entering the crystal. A general criterion for identifying the correlated detectors is proposed based on the equality of the signal intensities, and without involving the calculation of the joint detection probabilities. In addition, from the analyses in the rectilinear and diagonal basis, it is shown that the distinguishability of the polarisation Bell states, which is in direct correspondence with the joint detection events in each experiment, can be related to the knowledge of the phases of the vacuum field entering the entanglement source, and giving rise to correlated detections. To this purpose, it is conjectured that a detection event is associated with a maximum value of the signal intensity averaged in the modules of the zeropoint amplitudes, as a function of the vacuum phases. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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14 pages, 298 KiB  
Article
Quantum Oscillator at Temperature T and the Evolution of a Charged-Particle State in the Electric Field in the Probability Representation of Quantum Mechanics
by Margarita A. Man’ko and Vladimir I. Man’ko
Entropy 2023, 25(2), 213; https://doi.org/10.3390/e25020213 - 22 Jan 2023
Cited by 5 | Viewed by 1451
Abstract
A short review constructing the probability representation of quantum mechanics is given, and examples of the probability distributions describing the states of quantum oscillator at temperature T and the evolution of quantum states of a charged particle moving in the electric field of [...] Read more.
A short review constructing the probability representation of quantum mechanics is given, and examples of the probability distributions describing the states of quantum oscillator at temperature T and the evolution of quantum states of a charged particle moving in the electric field of an electrical capacitor are considered. Explicit forms of time-dependent integrals of motion, linear in the position and momentum, are used to obtain varying probability distributions describing the evolving states of the charged particle. Entropies corresponding to the probability distributions of initial coherent states of the charged particle are discussed. The relation of the Feynman path integral to the probability representation of quantum mechanics is established. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
16 pages, 334 KiB  
Article
Stochastic Particle Creation: From the Dynamical Casimir Effect to Cosmology
by Matías Mantiñan, Francisco D. Mazzitelli and Leonardo G. Trombetta
Entropy 2023, 25(1), 151; https://doi.org/10.3390/e25010151 - 11 Jan 2023
Cited by 3 | Viewed by 1384
Abstract
We study a stochastic version of the dynamical Casimir effect, computing the particle creation inside a cavity produced by a random motion of one of its walls. We first present a calculation perturbative in the amplitude of the motion. We compare the stochastic [...] Read more.
We study a stochastic version of the dynamical Casimir effect, computing the particle creation inside a cavity produced by a random motion of one of its walls. We first present a calculation perturbative in the amplitude of the motion. We compare the stochastic particle creation with the deterministic counterpart. Then, we go beyond the perturbative evaluation using a stochastic version of the multiple scale analysis, that takes into account stochastic parametric resonance. We stress the relevance of the coupling between the different modes induced by the stochastic motion. In the single-mode approximation, the equations are formally analogous to those that describe the stochastic particle creation in a cosmological context, that we rederive using multiple scale analysis. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
17 pages, 354 KiB  
Article
Invariant-Parameterized Exact Evolution Operator for SU(2) Systems with Time-Dependent Hamiltonian
by Hiromichi Nakazato, Alessandro Sergi, Agostino Migliore and Antonino Messina
Entropy 2023, 25(1), 96; https://doi.org/10.3390/e25010096 - 3 Jan 2023
Cited by 6 | Viewed by 1796
Abstract
We report the step-by-step construction of the exact, closed and explicit expression for the evolution operator U(t) of a localized and isolated qubit in an arbitrary time-dependent field, which for concreteness we assume to be a magnetic field. Our approach [...] Read more.
We report the step-by-step construction of the exact, closed and explicit expression for the evolution operator U(t) of a localized and isolated qubit in an arbitrary time-dependent field, which for concreteness we assume to be a magnetic field. Our approach is based on the existence of two independent dynamical invariants that enter the expression of SU(2) by means of two strictly related time-dependent, real or complex, parameters. The usefulness of our approach is demonstrated by exactly solving the quantum dynamics of a qubit subject to a controllable time-dependent field that can be realized in the laboratory. We further discuss possible applications to any SU(2) model, as well as the applicability of our method to realistic physical scenarios with different symmetry properties. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
13 pages, 2195 KiB  
Article
Superior Resilience of Non-Gaussian Entanglement against Local Gaussian Noises
by Sergey Filippov and Alena Termanova
Entropy 2023, 25(1), 75; https://doi.org/10.3390/e25010075 - 30 Dec 2022
Viewed by 1483
Abstract
Entanglement distribution task encounters a problem of how the initial entangled state should be prepared in order to remain entangled the longest possible time when subjected to local noises. In the realm of continuous-variable states and local Gaussian channels it is tempting to [...] Read more.
Entanglement distribution task encounters a problem of how the initial entangled state should be prepared in order to remain entangled the longest possible time when subjected to local noises. In the realm of continuous-variable states and local Gaussian channels it is tempting to assume that the optimal initial state with the most robust entanglement is Gaussian too; however, this is not the case. Here we prove that specific non-Gaussian two-mode states remain entangled under the effect of deterministic local attenuation or amplification (Gaussian channels with the attenuation factor/power gain κi and the noise parameter μi for modes i=1,2) whenever κ1μ22+κ2μ12<14(κ1+κ2)(1+κ1κ2), which is a strictly larger area of parameters as compared to where Gaussian entanglement is able to tolerate noise. These results shift the “Gaussian world” paradigm in quantum information science (within which solutions to optimization problems involving Gaussian channels are supposed to be attained at Gaussian states). Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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20 pages, 783 KiB  
Article
Adiabatic Amplification of the Harmonic Oscillator Energy When the Frequency Passes through Zero
by Viktor V. Dodonov and Alexandre V. Dodonov
Entropy 2023, 25(1), 2; https://doi.org/10.3390/e25010002 - 20 Dec 2022
Cited by 1 | Viewed by 1443
Abstract
We study the evolution of the energy of a harmonic oscillator when its frequency slowly varies with time and passes through a zero value. We consider both the classical and quantum descriptions of the system. We show that after a single frequency passage [...] Read more.
We study the evolution of the energy of a harmonic oscillator when its frequency slowly varies with time and passes through a zero value. We consider both the classical and quantum descriptions of the system. We show that after a single frequency passage through a zero value, the famous adiabatic invariant ratio of energy to frequency (which does not hold for a zero frequency) is reestablished again, but with the proportionality coefficient dependent on the initial state. The dependence on the initial state disappears after averaging over the phases of initial states with the same energy (in particular, for the initial vacuum, the Fock and thermal quantum states). In this case, the mean proportionality coefficient is always greater than unity. The concrete value of the mean proportionality coefficient depends on the power index of the frequency dependence on a time near the zero point. In particular, the mean energy triplicates if the frequency tends to zero linearly. If the frequency attains zero more than once, the adiabatic proportionality coefficient strongly depends on the lengths of time intervals between zero points, so that the mean energy behavior becomes quasi-stochastic after many passages through a zero value. The original Born–Fock theorem does not work after the frequency passes through zero. However, its generalization is found: the initial Fock state becomes a wide superposition of many Fock states, whose weights do not depend on time in the new adiabatic regime. When the mean energy triplicates, the initial Nth Fock state becomes a superposition of, roughly speaking, 6N states, distributed nonuniformly. The initial vacuum and low-order Fock states become squeezed, as well as the initial thermal states with low values of the mean energy. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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19 pages, 984 KiB  
Article
Exact Solution of a Time-Dependent Quantum Harmonic Oscillator with Two Frequency Jumps via the Lewis–Riesenfeld Dynamical Invariant Method
by Stanley S. Coelho, Lucas Queiroz and Danilo T. Alves
Entropy 2022, 24(12), 1851; https://doi.org/10.3390/e24121851 - 19 Dec 2022
Cited by 8 | Viewed by 3988
Abstract
Harmonic oscillators with multiple abrupt jumps in their frequencies have been investigated by several authors during the last decades. We investigate the dynamics of a quantum harmonic oscillator with initial frequency ω0, which undergoes a sudden jump to a frequency [...] Read more.
Harmonic oscillators with multiple abrupt jumps in their frequencies have been investigated by several authors during the last decades. We investigate the dynamics of a quantum harmonic oscillator with initial frequency ω0, which undergoes a sudden jump to a frequency ω1 and, after a certain time interval, suddenly returns to its initial frequency. Using the Lewis–Riesenfeld method of dynamical invariants, we present expressions for the mean energy value, the mean number of excitations, and the transition probabilities, considering the initial state different from the fundamental. We show that the mean energy of the oscillator, after the jumps, is equal or greater than the one before the jumps, even when ω1<ω0. We also show that, for particular values of the time interval between the jumps, the oscillator returns to the same initial state. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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14 pages, 1381 KiB  
Article
Extreme Electron Acceleration with Fixed Radiation Energy
by Michael R. R. Good, Chiranjeeb Singha and Vasilios Zarikas
Entropy 2022, 24(11), 1570; https://doi.org/10.3390/e24111570 - 31 Oct 2022
Cited by 7 | Viewed by 1600
Abstract
We examine the extreme situation of radiation from an electron that is asymptotically accelerated to the speed of light, resulting in finite emission energy. The analytic solution explicitly demonstrates the difference between radiation power loss and kinetic power loss (null). Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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Review

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17 pages, 366 KiB  
Review
Nonlocal Static and Dynamical Vacuum Field Correlations and Casimir–Polder Interactions
by Roberto Passante and Lucia Rizzuto
Entropy 2023, 25(10), 1424; https://doi.org/10.3390/e25101424 - 8 Oct 2023
Viewed by 823
Abstract
In this review, we investigate several aspects and features of spatial field correlations for the massless scalar field and the electromagnetic field, both in stationary and nonstationary conditions, and show how they manifest in two- and many-body static and dynamic dispersion interactions (van [...] Read more.
In this review, we investigate several aspects and features of spatial field correlations for the massless scalar field and the electromagnetic field, both in stationary and nonstationary conditions, and show how they manifest in two- and many-body static and dynamic dispersion interactions (van der Waals and Casimir–Polder). We initially analyze the spatial field correlations for noninteracting fields, stressing their nonlocal behavior, and their relation to two-body dispersion interactions. We then consider how field correlations are modified by the presence of a field source, such as an atom or in general a polarizable body, firstly in a stationary condition and then in a dynamical condition, starting from a nonstationary state. We first evaluate the spatial field correlation for the electric field in the stationary case, in the presence of a ground-state or excited-state atom, and then we consider its time evolution in the case of an initially nonstationary state. We discuss in detail their nonlocal features, in both stationary and nonstationary conditions. We then explicitly show how the nonlocality of field correlations can manifest itself in van der Waals and Casimir–Polder interactions between atoms, both in static and dynamic situations. We discuss how this can allow us to indirectly probe the existence and the properties of nonlocal vacuum field correlations of the electromagnetic field, a research subject of strong actual interest, also in consequence of recent measurements of spatial field correlations exploiting electro-optical sampling techniques. The subtle and intriguing relation between nonlocality and causality is also discussed. Full article
(This article belongs to the Special Issue Quantum Nonstationary Systems)
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