论文标题
在非马克维亚环境中挤压热状态的量子相干动力学
Quantum coherence dynamics of displaced squeezed thermal state in a Non-Markovian environment
论文作者
论文摘要
目前的工作中讨论了与外部浴室接触的位移挤压热状态的量子相干性的动力学行为。我们使用Fano-Anderson类型的汉密尔顿人来对环境进行建模并解决量子Langevin方程。从量子Langevin方程的解中,我们获得了绿色的功能,该功能用于计算正交操作员的期望值,而正交操作员的期望值又用于构造协方差矩阵。我们使用基于相对熵的度量来计算模式的量子相干性。对平均光子数的不同值进行了欧姆,亚欧姆和超级欧姆限制,研究了单模式的热状态。在所有这些限制中,我们发现,当系统和环境之间的耦合较弱时,相干性衰减并表现出马尔可夫的性质。当系统和环境紧密耦合时,我们观察到进化最初是马尔可夫人,一段时间后它变成了非马克维亚人。非马克维亚效应是由于对系统的环境反向作用造成的。最后,我们还介绍了在低温和高温方向上长期限制的连贯性的稳态动力学。我们发现,在低温和高温限制中,定性行为保持不变。但是定量值有所不同,因为系统中的相干性由于热反应而较低。
The dynamical behavior of quantum coherence of a displaced squeezed thermal state in contact with an external bath is discussed in the present work. We use a Fano-Anderson type of Hamiltonian to model the environment and solve the quantum Langevin equation. From the solution of the quantum Langevin equation we obtain the Green's functions which are used to calculate the expectation value of the quadrature operators which are in turn used to construct the covariance matrix. We use a relative entropy based measure to calculate the quantum coherence of the mode. The single mode squeezed thermal state is studied in the Ohmic, sub-Ohmic and the super-Ohmic limits for different values of the mean photon number. In all these limits, we find that when the coupling between the system and the environment is weak, the coherence decays monotonically and exhibit a Markovian nature. When the system and the environment are strongly coupled, we observe that the evolution is initially Markovian and after some time it becomes non-Markovian. The non-Markovian effect is due to the environmental back action on the system. Finally, we also present the steady state dynamics of the coherence in the long time limit in both low and high temperature regime. We find that the qualitative behavior remains the same in both the low and high temperature limits. But quantitative values differ because the coherence in the system is lower due to thermal decoherence.