Chakraborty Ahana, Sensarma Rajdeep
Department of Theoretical Physics, Tata Institute of Fundamental Research, Mumbai 400005, India.
Max Planck Institute for the Physics of Complex Systems, Nöthnitzerstrasse 38, 01187 Dresden, Germany.
Phys Rev Lett. 2021 Nov 12;127(20):200603. doi: 10.1103/PhysRevLett.127.200603.
We propose a new field theoretic method for calculating Renyi entropy of a subsystem of many interacting bosons without using replica methods. This method is applicable to dynamics of both open and closed quantum systems starting from arbitrary initial conditions. Our method identifies the Wigner characteristic of a reduced density matrix with the partition function of the whole system with a set of linear sources turned on only in the subsystem, and uses this to calculate the subsystem's Renyi entropy. We use this method to study the evolution of Renyi entropy in a noninteracting open quantum system starting from an initial Fock state. We find a relation between the initial state and final density matrix which determines whether the entropy shows nonmonotonic behavior in time. For non-Markovian dynamics, we show that the entropy approaches its steady-state value as a power law with exponents governed by nonanalyticities of the bath. We illustrate that this field-theoretic method can be used to study large bosonic open quantum systems.
我们提出了一种新的场论方法,用于计算许多相互作用玻色子子系统的雷尼熵,而无需使用复制方法。该方法适用于从任意初始条件开始的开放和封闭量子系统的动力学。我们的方法通过仅在子系统中打开一组线性源的整个系统的配分函数来识别约化密度矩阵的维格纳特征,并以此来计算子系统的雷尼熵。我们使用这种方法来研究从初始福克态开始的非相互作用开放量子系统中雷尼熵的演化。我们发现了初始态和最终密度矩阵之间的关系,该关系决定了熵在时间上是否表现出非单调行为。对于非马尔可夫动力学,我们表明熵以幂律形式趋近其稳态值,其指数由浴场的非解析性决定。我们举例说明这种场论方法可用于研究大型玻色子开放量子系统。