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Physica A Statistical Mechanics and its Applications

Statistical properties of a transformed Tavis-Cummings model

M. Sebawe Abdalla

Published Nov 1, 1991• 13 citations
Publisher
DOI
10.1016/0378-4371(91)90218-2

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Squeezing Property of Binomial State Field under the Anti-Tavis-Cummings Model

Hong‐Guang Piao

The interaction between two identical two-level atoms and single-mode binomial light field is studied in anti-Tavis-Cummings model,and the atoms stay in entangled state initially.When the classical field is strong enough,the interaction between the atoms and the light field can turn into an effective anti-Tavis-Cummings model and Tavis-Cummings model under the condition of large detuning.In this paper,we mainly probe into the squeezing property of the binomial state in anti-Tavis-Cummings model,and the influence of initial field parameters on the squeezing property of the field are discussed.The results show that the degree and period of squeezing depend strongly on the initial parameters,and energy nonconservation item has a great impact on squeezing property.

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Modelling many-body quantum dynamics with stochastic trajectories: a critical test on the Tavis-Cummings model

A. Leonau, S. Chuchurka, V. Sukharnikov +2 more

We critically explore the applicability of a recently proposed framework to sample the quantum dynamics of a many-body quantum system interacting with light by stochastic trajectories, applying it to the closed and open Tavis-Cummings model (TCM). The stochastic differential equations (SDEs) sample the positive P phase-space representation by analog complex-valued dynamical variables that are linked to the quantum operators. Statistical average over the stochastic trajectories yields the evolution of the quantum mechanical expectation values. However, numerical implementation of these SDEs for the TCM indicates divergent solutions, also known from other phase-space methods. This limits the applicability of the framework to finite propagation times, that are strongly dependent on the physical parameters and initial conditions of the system. We outline the underlying mathematical reason for these divergences and show that their contribution to the averages are, however, essential. To attempt to regularize the divergences, we transform the SDEs to an equivalent set of SDEs with different noise realisations, thereby pushing the valid time boundary. Quantum collapse and revival of the TCM, however, cannot be recovered by the stochastic trajectory approach, pointing to the general difficulty of the applicability of stochastic phase-space sampling methods to systems with strong quantum features.

quant-pharXiv:2511.08815•Nov 13, 2025•0 citations
The interaction between two identical two-level atoms and single-mode binomial light field is studied in anti-Tavis-Cummings model,and the atoms stay in entangled state initially.When the classical field is strong enough,the interaction between the atoms and the light field can turn into an effective anti-Tavis-Cummings model and Tavis-Cummings model under the condition of large detuning.In this paper,we mainly probe into the squeezing property of the binomial state in anti-Tavis-Cummings model,and the influence of initial field parameters on the squeezing property of the field are discussed.The results show that the degree and period of squeezing depend strongly on the initial parameters,and energy nonconservation item has a great impact on squeezing property.
We critically explore the applicability of a recently proposed framework to sample the quantum dynamics of a many-body quantum system interacting with light by stochastic trajectories, applying it to the closed and open Tavis-Cummings model (TCM). The stochastic differential equations (SDEs) sample the positive P phase-space representation by analog complex-valued dynamical variables that are linked to the quantum operators. Statistical average over the stochastic trajectories yields the evolution of the quantum mechanical expectation values. However, numerical implementation of these SDEs for the TCM indicates divergent solutions, also known from other phase-space methods. This limits the applicability of the framework to finite propagation times, that are strongly dependent on the physical parameters and initial conditions of the system. We outline the underlying mathematical reason for these divergences and show that their contribution to the averages are, however, essential. To attempt to regularize the divergences, we transform the SDEs to an equivalent set of SDEs with different noise realisations, thereby pushing the valid time boundary. Quantum collapse and revival of the TCM, however, cannot be recovered by the stochastic trajectory approach, pointing to the general difficulty of the applicability of stochastic phase-space sampling methods to systems with strong quantum features.