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Transient Energy Exchange and Quantum Resources in a Driven Five-Level Kerr Optomechanical Model

SYED ANWAR, M. Ibrahim Ibrahim, S. Abdul Khalik Khalik

Published Oct 23, 2026• 0 citations
Publisher

Abstract

Abstract We present a finite-time study of energy exchange, quantum correlations, work capacity, and phase sensitivity in a driven hybrid system composed of a five-level atom, a Kerr nonlinear optical mode, and a mechanical oscillator. The atom--field interaction is modulated periodically, while four local Lindblad channels describe two selected atomic transitions together with optical and mechanical damping. Rather than treating the dynamics as a completed heat-engine cycle, we analyze the system as a transient open quantum process and keep the different energetic and information-theoretic quantities clearly separated. The initial optical and mechanical states are taken to be displaced squeezed thermal states, and the atomic subsystem is prepared in a coherent superposition carrying a relative phase. We follow the total energy, reservoir-associated currents, signed driving work, total and reduced entropies, atom--rest negativity, local mechanical ergotropy, and the quantum Fisher information associated with the initial atomic phase. Four parameter sets are considered in order to identify how the Kerr-plus-shift term, atom--field coupling strength, and atomic temperature bias influence the finite-time response. The calculations also track the first-law residual and include selected solver, time-step, and Hilbert-space checks to assess numerical sensitivity without claiming uniform convergence for every parameter set. The results show that stronger atom--field coupling produces the largest sampled atom--rest negativity, but this increase in correlation does not lead to a comparable preservation of the reduced atomic phase quantum Fisher information. Within the employed finite truncation, removing the Kerr-plus-shift term changes the energy balance sufficiently to produce a small positive end-of-window signed work, whereas the other cases give negative final signed work. Because the zero-$\chi$ Hamiltonian has a formal high-occupation instability in the untruncated model and no dedicated enlarged-cutoff test was completed for that case, this small positive value is treated as a result conditional on the adopted finite truncation rather than as a converged engine-performance claim. The mechanical ergotropy remains a local state property and should not be identified with the work exchanged through the external modulation. Taken together, the results show that entanglement, metrological sensitivity, ergotropy, reservoir currents, and driving work respond differently to the same parameter changes. The conclusions therefore apply to the specified phenomenological finite-time model and should not be interpreted as evidence of a completed thermodynamic cycle or of a particular experimental implementation.

DOI
10.21203/rs.3.rs-11223219/v1

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Abstract We present a finite-time study of energy exchange, quantum correlations, work capacity, and phase sensitivity in a driven hybrid system composed of a five-level atom, a Kerr nonlinear optical mode, and a mechanical oscillator. The atom--field interaction is modulated periodically, while four local Lindblad channels describe two selected atomic transitions together with optical and mechanical damping. Rather than treating the dynamics as a completed heat-engine cycle, we analyze the system as a transient open quantum process and keep the different energetic and information-theoretic quantities clearly separated. The initial optical and mechanical states are taken to be displaced squeezed thermal states, and the atomic subsystem is prepared in a coherent superposition carrying a relative phase. We follow the total energy, reservoir-associated currents, signed driving work, total and reduced entropies, atom--rest negativity, local mechanical ergotropy, and the quantum Fisher information associated with the initial atomic phase. Four parameter sets are considered in order to identify how the Kerr-plus-shift term, atom--field coupling strength, and atomic temperature bias influence the finite-time response. The calculations also track the first-law residual and include selected solver, time-step, and Hilbert-space checks to assess numerical sensitivity without claiming uniform convergence for every parameter set. The results show that stronger atom--field coupling produces the largest sampled atom--rest negativity, but this increase in correlation does not lead to a comparable preservation of the reduced atomic phase quantum Fisher information. Within the employed finite truncation, removing the Kerr-plus-shift term changes the energy balance sufficiently to produce a small positive end-of-window signed work, whereas the other cases give negative final signed work. Because the zero-χ\chiχ Hamiltonian has a formal high-occupation instability in the untruncated model and no dedicated enlarged-cutoff test was completed for that case, this small positive value is treated as a result conditional on the adopted finite truncation rather than as a converged engine-performance claim. The mechanical ergotropy remains a local state property and should not be identified with the work exchanged through the external modulation. Taken together, the results show that entanglement, metrological sensitivity, ergotropy, reservoir currents, and driving work respond differently to the same parameter changes. The conclusions therefore apply to the specified phenomenological finite-time model and should not be interpreted as evidence of a completed thermodynamic cycle or of a particular experimental implementation.
Abstract We study phase-sensitive quantum dynamics in a hybrid cavity system consisting of a mov-ing four-level ladder atom, a quantized optical mode, and a mechanical oscillator. The atomicTransitions interact with the cavity field through a motion-dependent Jaynes-Cummings coupling.while radiation pressure couples the intracavity photons to the mechanical mode. A Kerr mediumprovides photon-number-dependent phase shifts, and an external magnetic field generates Zeeman-shifted atomic sublevels. The quantum Fisher information and the von Neumann entropy of thereduced atomic states are used to follow the redistribution of phase information and the generationof atom–environment correlations. The results show that stronger hybrid coupling generally trans-fers locally accessible phase information away from the atom while increasing the mixedness of theatomic subsystem. Since the full state evolves unitarily, the reduced atomic entropy also quantifiesthe entanglement between the atom and the combined field mechanics sector. Kerr nonlinearityreorganizes this information ‡flow and can produce delayed loss of phase sensitivity or partial recoveryseries at selected times. The work highlights why quantum Fisher information and von NeumannEntropy must be interpreted together when metrological usefulness and entanglement are studied.in hybrid light-matter systems.
Abstract In science and technology, precision measurement of physical quantities is crucial, and the quantum Fisher information (QFI) plays a significant role in the study of quantum systems. In this work, we explore the dynamics of QFI in a hybrid optomechanical system, which consists of a ♢-type four-level atom interacting with a single-mode quantized field via a multi-photon process. We account for various sources of dissipation, including the decay rates of the atom, the cavity and the mechanical modes. Using an effective Hamiltonian, we analytically derive the explicit form of the state vector of the entire system via the time-dependent Schrödinger equation. We then investigate the atomic QFI for the estimation precision of the decay rate of the mechanical oscillator. Furthermore, we examine how optomechanical and atom-field coupling strengths, dissipation parameters and multi-photon transition influence the dynamics of atomic QFI. Our numerical results suggest that the estimation precision of the decay rate of the mechanical oscillator can be controlled by these parameters.
The single-atom version of the quantum heat engine based on electromagnetically induced transparency is theoretically investigated in this paper. In contact with a hot and a cold bath, the atom trapped in an optical cavity is coherently coupled by a coherent field, thus generating photons as output through a process that mimics a heat engine. Using semiclassical theory, we obtain the conditions for the classical gain parameter being positive. Then by taking a full quantum approach, we discuss the statistical property of the generated photons depicted by the photon number distribution and Wigner function, and show that it can be effectively tuned by the coupling field. Investigations on the energy and entropy balances of the heat engine process lead to an interesting result that the power of the engine is simply the energy per time provided by the hot reservoir. The coupling field plays a critical role in supporting the heat-engine process. However, the energy that it provides is all dumped into the cold reservoir. The total energy exchange conforms to the first law of thermodynamics. The efficiency of the engine depends on the temperatures of the two reservoirs and the strength of the coupling field. The entropy change of the heat-engine process suggests that when working far above the threshold of lasing, the efficiency approaches that of its atomic-ensemble-based partner.
This study investigates the quantum dynamics of three-level Stark-shifted atomic systems under the influence of a Nonlinear Kerr Medium (NLKM), focusing on the interplay between Quantum Fisher Information (QFI), Von Neumann Entropy (VNE), and photon-mediated interactions. By analyzing the temporal evolution of QFI (quantifying parameter estimation precision) and VNE (measuring quantum entanglement (QE), we demonstrate how Kerr nonlinearity (χ), Stark shifts (β), phase (ϕ), and photon numbers govern system behavior. Key findings reveal that lower χ values (e.g., [Formula: see text]) induce oscillatory QFI decay and rapid VNE growth, driven by atomic motion and NLKM interactions, with QFI peaks inversely correlated to VNE dips. Higher [Formula: see text] stabilizes both metrics, suppressing decoherence and entanglement fluctuations. Elevated photon numbers enhance stability by strengthening field-atom correlations, reducing oscillation amplitudes (particularly at low χ), and mitigating quantum fluctuations. The Stark effect (SE) amplifies energy-level shifts, while phase adjustments introduce asymmetries in quantum interference. These results highlight the system's tunability via [Formula: see text], and photon density. They position it as a versatile platform for quantum metrology and information processing, where precision, entanglement stability, and photon-mediated coherence are critical. Kerr interactions suppress long-time coherence and entanglement, while when [Formula: see text], Stark shifts can induce mild, transient quantum correlations. These dynamics are essential for controlling entanglement in cavity QED systems, especially when precise metrological performance is desired.
Parametrically driven Kerr nonlinear quantum oscillator plays a central role in quantum optics, superconducting circuits, and in engineered light-matter interactions. For the development of future quantum technologies, it is crucial to understand the behavior of this quantum system under realistic dissipative conditions. The objective of this thesis is to investigate the phase-space dynamics of a dissipative Kerr nonlinear oscillator under different driving regimes and corresponding dissipation channels, with a particular focus on the emergence of nonclassical features in phase space. The aim is also to understand how nonlinearity and different driving mechanisms influence quantum properties such as coherence, nonclassicality, and phase-space structure. The analysis was carried out using the Wigner phase-space formalism and numerical simulations of the Lindblad master equation. The results show that in the case of finite nonlinearity the coherence time is prolonged compared to the harmonic case. In the single photon regime, the interplay between the photon drive and nonlinearity can lead to coherence revivals after which the system relaxes into a squeezed steady state. In the two photon and dissipation regime, the system exhibits parity-protected dynamics, leading to very long coherence times.
Optomechanical cavity is a powerful connection between a nanomechanical oscillator and a quantized electromagnetic field. In this system, a novel photon-phonon nonlinear interaction arising from the nanomechanical oscillation is produced through the radiation pressure. Now this nonlinear photon-phonon interaction has become an important resource for implementing high-precision measurements and processing quantum information. Motivated by T. Esslinger group’s experiment, it is very meaningful to explore the exotic quantum phenomena when a ultra-cold BEC is trapped in an optomechanical cavity. In this paper, we mainly investigate phase transition and the finite-temperature thermodynamic properties of a Bose-Einstein condensate in an optomechanical cavity. It’s worth mentioning that at zero temperature many different mean-field approximate methods have been used to analyze the ground state properties of a Bose-Einstein condensate in an optomechanical cavity. Two common methods are Holstein-Primakoff transformation and spin coherent state variation. In this paper, an interesting imaginary-time path integral approach has been introduced to study finite temperature thermodynamic properties and phase transition of a Bose-Einstein condensate in an optomechanical cavity. First, we obtained system's partition function by taking imaginary-time path integration. Meanwhile, an effective action has been obtained by means of this method, which is the basic of the variation to get the numerical solution of photon number and the expression of the atomic number. At zero temperature, these results are consistent with what we have obtained by Holstein-Primakoff transformation or spin coherent state variational method. By adjusting the atom-field coupling strength and other parameters the second-order phase transition from the normal phase to the superradiant phase has been revealed. Meanwhile, a new unstable superradiant state was also found. And we found that in addition to the normal phase and superradiation phase, there exists an un-solution region of the mean photon number. Meanwhile, we find that the nonlinear photon-phonon interaction does not affect the normal phase. However, in the superradiant phase, the nonlinear photon-phonon interaction can enhance the macroscopic collective excitations. At the same time, the thermodynamic properties of the system are also discussed. According to the obtained distribution function, we can derive the analytical expression of the average energy and the free energy. Furthermore, the expression of entropy at finite temperature can also be obtained. we find the nonlinear photon-phonon interaction does not affect the average energy in the normal phase, but the average energy in the superradiant phase can deeply deviate in the large nonlinear photon-phonon interaction. It’s worth mentioning that the mean photon number and average energy in the finite-temperature tend to be consistent with the case in absolute zero temperature in the strong coupling region, while the entropy in the superradiant phase is rapidly reduced to zero as the atom-field coupling strength increases. In other words, strongly coupled collective excited states are highly ordered and are not affected by thermal fluctuations in the temperature range we are considering. The thermodynamic properties, such as the entropy and corresponding specific heat, characterize the Dicke phase transition.