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arXiv 2609.18208cond-mat.stat-mech

自由费米子动力学量子相变中的对数奇异性

Logarithmic singularity in a dynamical quantum phase transition for free fermions

发表机构伯明翰大学 · 圣塔菲研究所 · 巴黎萨克雷大学
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  • University of Birmingham(伯明翰大学)
  • Santa Fe Institute(圣塔菲研究所)
  • Université Paris-Saclay(巴黎萨克雷大学)
  • Université de Toulouse(图卢兹大学)

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Yasser Bezzaz, Dimitri M. Gangardt, Pavel L. Krapivsky, Jean-Marc Luck, Kirone Mallick, Sylvain Prolhac

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中文总结 AI 辅助

本研究通过Loschmidt回声研究自由费米子系统的动力学量子相变,发现动力学自由能出现对数奇异性,并将其解释为瞬子构型的拓扑变化,且后选择可驱动两次连续相变。

中文摘要 AI 辅助

我们研究了从双畴壁初始态释放的N个无相互作用无自旋格点费米子系统中的Loschmidt回声。在大N极限下,返回概率由大偏差率函数表征,该函数称为动力学自由能。Loschmidt回声由复瞬子构型主导,动力学自由能在动力学量子相变处发展出对数奇异性。我们获得了短时间和长时间区域的解析结果,并通过数值计算加以验证。我们表明,该相变可以理解为占主导地位的瞬子构型的拓扑变化,类似于随机矩阵理论中割线的出现。我们进一步表明,后选择可以驱动系统经历两次连续的动力学量子相变(DQPT),这些相变与复时间中占主导地位的瞬子构型的连续拓扑变化相关。

英文摘要

We study the Loschmidt echo in a system of N non-interacting spinless lattice fermions released from a double-domain-wall initial state. In the large-N limit, the return probability is characterized by a large-deviation rate function known as the dynamical free energy. The Loschmidt echo is dominated by a complex instanton configuration, and the dynamical free energy develops a logarithmic singularity at the dynamical quantum phase transition. We obtain analytical results in the short-time and long-time regimes and support them with numerical computations. We show that the transition can be understood as a topological change of the dominant instanton configuration, analogous to the emergence of a cut in random matrix theory. We further show that post-selection can drive the system through two successive DQPTs, associated with successive topological changes of the dominant instanton configuration in complex time.

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