Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1606.08235 · Physical Review A

Dynamics of a quantum two-state system in a linearly driven quantum bath

Joscha Reichert, P. Nalbach, Michael Thorwart

Published Sep 28, 2016• 12 citations
arXivHTMLPDF

Abstract

When an open quantum system is driven by an external time-dependent force, the coupling of the driving to the central system is usually included, whereas the impact of the driving field on the bath is neglected. We investigate the effect of a quantum bath of linearly driven harmonic oscillators on the relaxation dynamics of a quantum two-level system which is not directly driven. In particular, we calculate the frequency-dependent response of the system when the bath is subject to Dirac and Gaussian driving pulses. We show that a time-retarded effective force on the system is induced by the driven bath which depends on the full history of the perturbation and the spectral characteristics of the underlying bath. In particular, when a structured Ohmic bath with a pronounced Lorentzian peak is considered, the dynamical response of the system to a driven bath is qualitatively different than that of the undriven bath. Specifically, additional resonances appear which can be directly associated with a Jaynes-Cummings-like effective energy spectrum.

DOI
10.1103/physreva.94.032127

Related papers

Quantum mechanical response to a driven Caldeira-Leggett bath

Hermann Grabert, Michael Thorwart

We determine the frequency-dependent response characteristics of a quantum system to a driven Caldeira-Leggett bath. The bath degrees of freedom are explicitly driven by an external time-dependent force, in addition to the direct time-dependent forcing of the system itself. After general considerations of driven Caldeira-Leggett baths, we consider the Rubin model of a chain of quantum particles coupled by linear springs as an important model of a quantum dissipative system. We show that in the presence of time-dependent driving of the chain, this model can be mapped to a quantum system which couples to a driven Caldeira-Leggett bath. The effect of the bath driving is captured by a time-dependent force on the central system, which is, in principle, non-Markovian in nature. We study two specific examples, the exactly solvable case of a harmonic potential and a quantum two-state system for which we assume a weak system-bath coupling. We evaluate the dynamical response to a periodic driving of the system and the bath. The dynamic susceptibility is shown to be altered qualitatively by the bath drive: The dispersive part is enhanced at low frequencies and acquires a maximum at zero frequency. The absorptive part develops a shoulder-like behavior in this frequency regime. These features seem to be generic for quantum systems in a driven Caldeira-Leggett bath.

arXiv:1807.01557•Physical review. E•Jul 17, 2018•22 citations

The Physical Spectrum of a Driven Jaynes–Cummings Model

L. Medina-Dozal, Alejandro R. Urzúa, I. Ramos-Prieto +4 more

We analyze the time-dependent physical spectrum of a driven Jaynes-Cummings model in which both the two-level system and the quantized cavity mode are subject to coherent classical driving. The time-dependent Hamiltonian is mapped, via well-defined unitary transformations, onto an effective stationary Jaynes-Cummings form. Within this framework, we derive closed-form expressions for the two-time correlation functions of both the atomic and field operators. These correlation functions are subsequently used to evaluate the time-dependent physical spectrum according to the Eberly-Wódkiewicz definition, which properly accounts for finite spectral resolution and transient emission dynamics. We show that the external driving leads to substantial modifications of the atomic spectral response, including controllable frequency shifts and asymmetric line shapes. Importantly, we identify a regime in which the driving parameters are chosen such that the coherent displacement induced in the cavity field exactly cancels out the initial coherent amplitude. In this limit, the system dynamics reduce to that of an effectively vacuum-initialized Jaynes-Cummings model, and the standard vacuum Rabi splitting is recovered. This behavior provides a clear and physically transparent interpretation of the spectral features as arising from coherent field displacement rather than from modifications of the underlying atom-cavity coupling.

Entropy•Jan 21, 2026•1 citation

Dynamics of a qubit coupled to a dissipative nonlinear quantum oscillator: An effective-bath approach

Carmen Vierheilig, Dario Bercioux, Milena Grifoni

We consider a qubit coupled to a nonlinear quantum oscillator, the latter coupled to an Ohmic bath, and investigate the qubit dynamics. This composed system can be mapped onto that of a qubit coupled to an effective bath. An approximate mapping procedure to determine the spectral density of the effective bath is given. Specifically, within a linear response approximation the effective spectral density is given by knowledge of the linear susceptibility of the nonlinear quantum oscillator. To determine the actual form of the susceptibility, we consider its periodically driven counterpart, which is the problem of the quantum Duffing oscillator within linear response theory in the driving amplitude. Knowing the effective spectral density, the qubit dynamics is investigated. In particular, an analytic formula for the qubit's population difference is derived. Within the regime of validity of our theory, a very good agreement is found with predictions obtained from a Bloch-Redfield master equation approach applied to the composite qubit-nonlinear oscillator system.

arXiv:1010.4684•Physical Review A•Jan 18, 2011•10 citations

Dissipative dynamics of a biased qubit coupled to a harmonic oscillator: Analytical results beyond the rotating wave approximation

Johannes Hausinger, Milena Grifoni

We study the dissipative dynamics of a biased two-level system (TLS) coupled to a harmonic oscillator (HO), the latter interacting with an Ohmic environment. Using Van-Vleck perturbation theory and going to second order in the coupling between TLS and HO, we show how the Hamiltonian of the TLS-HO system can be diagonalized analytically. Our model represents an improvement to the usually used Jaynes-Cummings Hamiltonian as an initial rotating wave approximation is avoided. By assuming a weak coupling to the thermal bath, analytical expressions for the time evolution of the populations of the TLS are\nfound: the population is characterized by a multiplicity of damped oscillations together with a complex relaxation dynamics towards thermal equilibrium. The long time evolution is characterized by a single relaxation rate, which is largest at resonance and whose expression can be given in closed analytic form.

•Jan 1, 2008•43 citations

Dissipative dynamics of a biased qubit coupled to a harmonic oscillator: analytical results beyond the rotating wave approximation

Johannes Hausinger, Milena Grifoni

We study the dissipative dynamics of a biased two-level system (TLS) coupled to a harmonic oscillator (HO), the latter interacting with an Ohmic environment. Using the Van Vleck perturbation theory and going to second order in the coupling between the TLS and the HO, we show how the Hamiltonian of the TLS–HO system can be diagonalized analytically. Our model represents an improvement on the usually used Jaynes–Cummings Hamiltonian as an initial rotating wave approximation is avoided. By assuming a weak coupling to the thermal bath, analytical expressions for the time evolution of the populations of the TLS are found: the population is characterized by a multiplicity of damped oscillations together with a complex relaxation dynamics towards thermal equilibrium. The long time evolution is characterized by a single relaxation rate, which is largest at resonance and whose expression can be given in a closed analytic form.

arXiv:0806.3387•New Journal of Physics•Nov 20, 2008•46 citations

Resonance-Dependent Dynamics in Driven Quantum Systems: A Normalized Simulation Framework for Frequency Sweeps, Phase Space Response, and Level Modeling

Dimosthenis K. Michopoulos, Spyridon K. Chronopoulos, Kostas P. Peppas

Abstract Externally driven quantum systems, operating under sensitive conditions of resonance, constitute an important class of physical platforms in quantum technologies, superconducting resonant architectures, and Josephson-junction-based environments. In this class of systems, an externally imposed electromagnetic driving frequency may influence oscillatory dynamics, coherence, spectral structure, and the frequency-dependent energy distribution. This work proposes an exploratory theoretical framework for interpreting resonance-dependent energy and spectral distributions in externally driven quantum systems, treating the driving frequency not only as an external perturbation but also as an active configuration parameter of the system's response. In the proposed formulation, resonance-sensitive behavior is described through a normalized resonance-response function. The formulation distinguishes between the non-driven reference spectrum and the externally driven effective spectrum, where resonance-dependent level shifts appear as deviations from the non-driven case. Two quantities, denoted by Λ and Δ, are introduced to describe the energy distribution associated with the externally driven response. Within the proposed interpretation, Λ represents the averaged potential and externally driven contribution, while Δ represents a cycle-averaged energy of the driven response. These quantities are not intended to replace the standard Hamiltonian description of quantum systems, but to provide an additional clarifying way to analyze how externally imposed conditions in resonance may reorganize effective energetic and spectral behavior. The proposed approach is relevant to periodically driven quantum systems, Floquet-type spectral descriptions (interpreting frequency-induced modifications), superconducting resonant environments, and Josephson-junction-based systems, while remaining complementary to standard time-dependent quantum and superconducting-circuit formulations. To support the theoretical interpretation, numerical simulations are presented for three representative microwave resonance areas at 6.1, 6.9, and 7.7 GHz. The simulations employ a normalized resonance-response function and include resonance-response profiles, spectral analysis, effective energy spectra, phase-space trajectories, averaged energy-distribution components, and Gaussian probability-density maps. Additional local- and global-sweep methodology relevant to phase-space simulations further illustrate how frequency deviation from resonance and externally imposed frequency variation may reshape the distribution of phase-space activity. The simulated trajectories represent the phase-space evolution of position and momentum coordinates in a driven-oscillator model, rather than literal quantum particle paths. Similarly, the Josephson effect motivated the use of microwave frequency sweeps, since driven Josephson systems exhibit phase-sensitive and resonance-dependent behavior. Therefore, the frequency-sweep simulations should be interpreted as a preparatory resonance-response analysis, rather than as a full Josephson model. The results suggest that resonance-dependent spectral and phase-space distribution may provide useful qualitative insight for frequency-controlled quantum systems, superconducting resonant architectures, and resonance-sensitive or control platforms. This study is intended as an exploratory theoretical and simulation-based contribution, presenting how externally controlled resonance conditions influence phase-space dynamics in driven quantum systems.

•Jun 22, 2026•0 citations
When an open quantum system is driven by an external time-dependent force, the coupling of the driving to the central system is usually included, whereas the impact of the driving field on the bath is neglected. We investigate the effect of a quantum bath of linearly driven harmonic oscillators on the relaxation dynamics of a quantum two-level system which is not directly driven. In particular, we calculate the frequency-dependent response of the system when the bath is subject to Dirac and Gaussian driving pulses. We show that a time-retarded effective force on the system is induced by the driven bath which depends on the full history of the perturbation and the spectral characteristics of the underlying bath. In particular, when a structured Ohmic bath with a pronounced Lorentzian peak is considered, the dynamical response of the system to a driven bath is qualitatively different than that of the undriven bath. Specifically, additional resonances appear which can be directly associated with a Jaynes-Cummings-like effective energy spectrum.
We determine the frequency-dependent response characteristics of a quantum system to a driven Caldeira-Leggett bath. The bath degrees of freedom are explicitly driven by an external time-dependent force, in addition to the direct time-dependent forcing of the system itself. After general considerations of driven Caldeira-Leggett baths, we consider the Rubin model of a chain of quantum particles coupled by linear springs as an important model of a quantum dissipative system. We show that in the presence of time-dependent driving of the chain, this model can be mapped to a quantum system which couples to a driven Caldeira-Leggett bath. The effect of the bath driving is captured by a time-dependent force on the central system, which is, in principle, non-Markovian in nature. We study two specific examples, the exactly solvable case of a harmonic potential and a quantum two-state system for which we assume a weak system-bath coupling. We evaluate the dynamical response to a periodic driving of the system and the bath. The dynamic susceptibility is shown to be altered qualitatively by the bath drive: The dispersive part is enhanced at low frequencies and acquires a maximum at zero frequency. The absorptive part develops a shoulder-like behavior in this frequency regime. These features seem to be generic for quantum systems in a driven Caldeira-Leggett bath.
We analyze the time-dependent physical spectrum of a driven Jaynes-Cummings model in which both the two-level system and the quantized cavity mode are subject to coherent classical driving. The time-dependent Hamiltonian is mapped, via well-defined unitary transformations, onto an effective stationary Jaynes-Cummings form. Within this framework, we derive closed-form expressions for the two-time correlation functions of both the atomic and field operators. These correlation functions are subsequently used to evaluate the time-dependent physical spectrum according to the Eberly-Wódkiewicz definition, which properly accounts for finite spectral resolution and transient emission dynamics. We show that the external driving leads to substantial modifications of the atomic spectral response, including controllable frequency shifts and asymmetric line shapes. Importantly, we identify a regime in which the driving parameters are chosen such that the coherent displacement induced in the cavity field exactly cancels out the initial coherent amplitude. In this limit, the system dynamics reduce to that of an effectively vacuum-initialized Jaynes-Cummings model, and the standard vacuum Rabi splitting is recovered. This behavior provides a clear and physically transparent interpretation of the spectral features as arising from coherent field displacement rather than from modifications of the underlying atom-cavity coupling.
We consider a qubit coupled to a nonlinear quantum oscillator, the latter coupled to an Ohmic bath, and investigate the qubit dynamics. This composed system can be mapped onto that of a qubit coupled to an effective bath. An approximate mapping procedure to determine the spectral density of the effective bath is given. Specifically, within a linear response approximation the effective spectral density is given by knowledge of the linear susceptibility of the nonlinear quantum oscillator. To determine the actual form of the susceptibility, we consider its periodically driven counterpart, which is the problem of the quantum Duffing oscillator within linear response theory in the driving amplitude. Knowing the effective spectral density, the qubit dynamics is investigated. In particular, an analytic formula for the qubit's population difference is derived. Within the regime of validity of our theory, a very good agreement is found with predictions obtained from a Bloch-Redfield master equation approach applied to the composite qubit-nonlinear oscillator system.
We study the dissipative dynamics of a biased two-level system (TLS) coupled to a harmonic oscillator (HO), the latter interacting with an Ohmic environment. Using Van-Vleck perturbation theory and going to second order in the coupling between TLS and HO, we show how the Hamiltonian of the TLS-HO system can be diagonalized analytically. Our model represents an improvement to the usually used Jaynes-Cummings Hamiltonian as an initial rotating wave approximation is avoided. By assuming a weak coupling to the thermal bath, analytical expressions for the time evolution of the populations of the TLS are\nfound: the population is characterized by a multiplicity of damped oscillations together with a complex relaxation dynamics towards thermal equilibrium. The long time evolution is characterized by a single relaxation rate, which is largest at resonance and whose expression can be given in closed analytic form.
We study the dissipative dynamics of a biased two-level system (TLS) coupled to a harmonic oscillator (HO), the latter interacting with an Ohmic environment. Using the Van Vleck perturbation theory and going to second order in the coupling between the TLS and the HO, we show how the Hamiltonian of the TLS–HO system can be diagonalized analytically. Our model represents an improvement on the usually used Jaynes–Cummings Hamiltonian as an initial rotating wave approximation is avoided. By assuming a weak coupling to the thermal bath, analytical expressions for the time evolution of the populations of the TLS are found: the population is characterized by a multiplicity of damped oscillations together with a complex relaxation dynamics towards thermal equilibrium. The long time evolution is characterized by a single relaxation rate, which is largest at resonance and whose expression can be given in a closed analytic form.
Abstract Externally driven quantum systems, operating under sensitive conditions of resonance, constitute an important class of physical platforms in quantum technologies, superconducting resonant architectures, and Josephson-junction-based environments. In this class of systems, an externally imposed electromagnetic driving frequency may influence oscillatory dynamics, coherence, spectral structure, and the frequency-dependent energy distribution. This work proposes an exploratory theoretical framework for interpreting resonance-dependent energy and spectral distributions in externally driven quantum systems, treating the driving frequency not only as an external perturbation but also as an active configuration parameter of the system's response. In the proposed formulation, resonance-sensitive behavior is described through a normalized resonance-response function. The formulation distinguishes between the non-driven reference spectrum and the externally driven effective spectrum, where resonance-dependent level shifts appear as deviations from the non-driven case. Two quantities, denoted by Λ and Δ, are introduced to describe the energy distribution associated with the externally driven response. Within the proposed interpretation, Λ represents the averaged potential and externally driven contribution, while Δ represents a cycle-averaged energy of the driven response. These quantities are not intended to replace the standard Hamiltonian description of quantum systems, but to provide an additional clarifying way to analyze how externally imposed conditions in resonance may reorganize effective energetic and spectral behavior. The proposed approach is relevant to periodically driven quantum systems, Floquet-type spectral descriptions (interpreting frequency-induced modifications), superconducting resonant environments, and Josephson-junction-based systems, while remaining complementary to standard time-dependent quantum and superconducting-circuit formulations. To support the theoretical interpretation, numerical simulations are presented for three representative microwave resonance areas at 6.1, 6.9, and 7.7 GHz. The simulations employ a normalized resonance-response function and include resonance-response profiles, spectral analysis, effective energy spectra, phase-space trajectories, averaged energy-distribution components, and Gaussian probability-density maps. Additional local- and global-sweep methodology relevant to phase-space simulations further illustrate how frequency deviation from resonance and externally imposed frequency variation may reshape the distribution of phase-space activity. The simulated trajectories represent the phase-space evolution of position and momentum coordinates in a driven-oscillator model, rather than literal quantum particle paths. Similarly, the Josephson effect motivated the use of microwave frequency sweeps, since driven Josephson systems exhibit phase-sensitive and resonance-dependent behavior. Therefore, the frequency-sweep simulations should be interpreted as a preparatory resonance-response analysis, rather than as a full Josephson model. The results suggest that resonance-dependent spectral and phase-space distribution may provide useful qualitative insight for frequency-controlled quantum systems, superconducting resonant architectures, and resonance-sensitive or control platforms. This study is intended as an exploratory theoretical and simulation-based contribution, presenting how externally controlled resonance conditions influence phase-space dynamics in driven quantum systems.