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arXiv 2308.04495quant-phcond-mat.str-elphysics.optics
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非厄米准晶体中关联粒子的相变与聚集

Phase transitions and bunching of correlated particles in a non-Hermitian quasicrystal

Stefano Longhi

AI总结:

本文研究非厄米准晶体中两个相互作用粒子的谱学与动力学,发现doublon态因关联跃迁减弱而具有更低的相变阈值和更长寿命,导致粒子在长时间演化中自发聚集形成束缚态。

摘要:

非厄米准晶体中的非相互作用粒子在复能量平面中表现出局域-退局域化转变和谱相变,这些现象可以通过点隙拓扑来表征。本文研究了一个非厄米准晶体中两个相互作用粒子的谱学与动力学特征,该系统由一个具有复相位的不公度正弦势中的有效Hubbard模型描述,并揭示了一些没有任何厄米对应物的有趣效应。由于粒子相互作用引入了关联跃迁的有效减小,doublon态(即束缚粒子态)表现出比单粒子态低得多的谱转变和局域-退局域化转变阈值,从而导致迁移率边的出现。值得注意的是,由于doublon具有更长的寿命,初始放置在远距离格点上的两个粒子倾向于聚集并粘合在一起,在长时间演化极限下形成doublon态,这一现象可以被称为非厄米粒子聚集。

英文摘要:

Non-interacting particles in non-Hermitian quasi crystals display localization-delocalization and spectral phase transitions in complex energy plane, that can be characterized by point-gap topology. Here we investigate the spectral and dynamical features of two interacting particles in a non-Hermitian quasi crystal, described by an effective Hubbard model in an incommensurate sinusoidal potential with a complex phase, and unravel some intriguing effects without any Hermitian counterpart. Owing to the effective decrease of correlated hopping introduced by particle interaction, doublon states, i.e. bound particle states, display a much lower threshold for spectral and localization-delocalization transitions than single-particle states, leading to the emergence of mobility edges. Remarkably, since doublons display longer lifetimes, two particles initially placed in distant sites tend to bunch and stick together, forming a doublon state in the long time limit of evolution, a phenomenon that can be dubbed {\em non-Hermitian particle bunching}.

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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