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Thermalization of strongly interacting bosons after spontaneous emissions in optical lattices

机译:光学晶格中自发发射后强相互作用的玻色子的热化

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Abstract We study the out-of-equilibrium dynamics of bosonic atoms in a 1D optical lattice, after the ground-state is excited by a single spontaneous emission event, i.e. after an absorption and re-emission of a lattice photon. This is an important fundamental source of decoherence for current experiments, and understanding the resulting dynamics and changes in the many-body state is important for controlling heating in quantum simulators. Previously it was found that in the superfluid regime, simple observables relax to values that can be described by a thermal distribution on experimental time-scales, and that this breaks down for strong interactions (in the Mott insulator regime). Here we expand on this result, investigating the relaxation of the momentum distribution as a function of time, and discussing the relationship to eigenstate thermalization. For the strongly interacting limit, we provide an analytical analysis for the behavior of the system, based on an effective low-energy Hamiltonian in which the dynamics can be understood based on correlated doublon-holon pairs.
机译:摘要我们研究了一维光学晶格中的硼原子的失衡动力学,该基态由单个自发发射事件激发,即在吸收和重新发射晶格光子后激发了基态。对于当前的实验来说,这是一个重要的基本退相干源,了解由此产生的动力学和多体状态变化对于控制量子模拟器中的加热非常重要。先前发现,在超流体状态下,简单的可观测值松弛到可以通过实验时标上的热分布描述的值,并且由于强相互作用而分解(在莫特绝缘子状态下)。在这里,我们对这个结果进行扩展,研究作为时间函数的动量分布的松弛,并讨论与本征态热化的关系。对于强烈相互作用的限制,我们基于有效的低能量哈密顿量提供了系统行为的分析分析,其中基于相关的杜布隆-霍隆对可了解动力学。

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