Theoretical methods to treat a single dissipative bosonic mode coupled globally to an interacting many-body system

C. Halati, A. Sheikhan, C. Kollath
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引用次数: 5

Abstract

We present two approaches capable of describing the dynamics of an interacting many body system on a lattice coupled globally to a dissipative bosonic mode. Physical realizations are for example ultracold atom gases in optical lattice coupled to a photonic mode of an optical cavity or electronic gases in solids coupled to THz cavity fields. The first approach, applicable for large dissipation strengths and any system size, is a variant of the many-body adiabatic elimination method for investigating the long time dynamics of the system. The second method extends the time-dependent matrix product techniques to capture the global coupling of the interacting particles to the bosonic mode and its open nature. It gives numerically exact results for small to intermediate system sizes. As a benchmark for our methods we perform the full quantum evolution of a Bose-Hubbard chain coupled to a cavity mode. We show that important deviations from the mean field behavior occur when considering the full atoms cavity coupling [1].
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处理全局耦合到相互作用多体系统的单耗散玻色子模的理论方法
我们提出了两种能够描述晶格上与耗散玻色子模式耦合的相互作用多体系统动力学的方法。例如,物理实现是光学晶格中的超冷原子气体耦合到光学腔的光子模式或固体中的电子气体耦合到太赫兹腔场。第一种方法是用于研究系统长时间动力学的多体绝热消去法的一种变体,适用于大耗散强度和任何系统尺寸。第二种方法扩展了时变矩阵积技术,以捕获相互作用粒子对玻色子模式及其开放性质的全局耦合。它给出了小到中等系统尺寸的精确数值结果。作为我们方法的基准,我们执行了玻色-哈伯德链耦合到腔模式的全量子演化。我们表明,当考虑全原子腔耦合时,会发生与平均场行为的重要偏差。
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