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Nonequilibrium phase diagram of a driven and dissipative many-body system

机译:驱动和耗散多体系统的非平衡相图

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We study the nonequilibrium dynamics of a many-body bosonic system on a lattice, subject to driving and dissipation. The time evolution is described by a master equation, which we treat within a generalized Gutzwiller mean field approximation for density matrices. The dissipative processes are engineered such that the system, in the absence of interaction between the bosons, is driven into a homogeneous steady state with off-diagonal long-range order. We investigate how the coherent interaction affects the properties of the steady state of the system qualitatively and derive a nonequilibrium phase diagram featuring a phase transition into a steady state without long-range order. The phase diagram also exhibits an extended domain where an instability of the homogeneous steady state gives rise to a persistent density pattern with spontaneously broken translational symmetry. In the limit of low particle density, we provide a precise analytical description of the time evolution during the instability. Moreover, we investigate the transient following a quantum quench of the dissipative processes and we elucidate the prominent role played by collective topological variables in this regime.
机译:我们研究了受驱动和耗散作用的晶格上多体玻色子系统的非平衡动力学。时间演化由一个主方程描述,我们在密度矩阵的广义Gutzwiller平均场近似中对其进行处理。对耗散过程进行了设计,使得在玻色子之间不存在相互作用的情况下,系统以偏离对角线的远距离顺序被驱动到均匀的稳态。我们研究相干相互作用如何定性地影响系统稳态的性质,并推导了一个非平衡相图,该相图具有从相态过渡到无长程稳态的稳态。相图还展示了一个扩展域,其中均匀稳态的不稳定性导致了自发破坏的平移对称性的持续密度模式。在低颗粒密度的限制下,我们提供了不稳定过程中时间演化的精确分析描述。此外,我们研究了耗散过程的量子猝灭后的瞬态,并阐明了该拓扑中集体拓扑变量所扮演的重要角色。

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