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arXiv 2305.04643quant-phcond-mat.stat-mech
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弛豫时间作为探索动力学相图的控制参数

Relaxation time as a control parameter for exploring dynamical phase diagrams

Ángel L. Corps, Pedro Pérez-Fernández, Armando Relaño

AI总结:

本文提出以弛豫时间为唯一控制参数的双重淬火协议,应用于非谐Lipkin-Meshkov-Glick模型,利用守恒量刻画了由两个激发态量子相变导致的多种动力学相变。

摘要:

我们通过一种双重淬火协议探索完整的动力学相图,该协议以弛豫时间作为唯一的控制参数。该协议包含两次固定的淬火以及一个中间的弛豫时间,后者决定了最终淬火后量子态所处的相。我们将其应用于一个非谐的Lipkin-Meshkov-Glick模型。该模型展现出两个激发态量子相变,将谱分为三个不同的相:其中两个是对称破缺相,一个是无序相。因此,我们的协议诱导出多种动力学相变。我们根据表征模型所有三个相的守恒量来刻画所有这些动力学相变。

英文摘要:

We explore a full dynamical phase diagram by means of a double quench protocol that depends on a relaxation time as the only control parameter. The protocol comprises two fixed quenches and an intermediate relaxation time that determines the phase in which the quantum state is placed after the final quench. We apply it to an anharmonic Lipkin-Meshkov-Glick model. This model displays two excited-state quantum phase transitions which split the spectrum into three different phases: two of them are symmetry-breaking phases, and one is a disordered phase. As a consequence, our protocol induces several kind of dynamical phase transitions. We characterize all of them in terms of the constants of motion characterizing all three phases of the model.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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