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arXiv 1905.13232cond-mat.str-elcond-mat.dis-nncond-mat.quant-gascond-mat.stat-mech
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离散时间晶体

Discrete Time Crystals

Dominic V. Else, Christopher Monroe, Chetan Nayak, Norman Y. Yao

摘要:

实验的进步已经允许探索几乎孤立的量子多体系统,其与外部浴的耦合非常弱。一类特别有趣的系统是那些在自己的孤立量子动力学下不热化的系统。在这篇综述中,我们强调了这种系统表现出新的非平衡态物质相的可能性。特别是,我们专注于“离散时间晶体”,这是多体相位的物质,其特征在于自发打破离散时间平移对称性。本文从几个角度给出了离散时间晶体的定义,强调离散时间晶体是一种非平衡现象,它是由多体相互作用稳定的,在非相互作用系统中没有类似的现象。我们解释了几种离散时间晶体模型背后的理论,并比较了一些最近的实现,在不同的实验环境。

英文摘要:

Experimental advances have allowed for the exploration of nearly isolated quantum many-body systems whose coupling to an external bath is very weak. A particularly interesting class of such systems is those which do not thermalize under their own isolated quantum dynamics. In this review, we highlight the possibility for such systems to exhibit new non-equilibrium phases of matter. In particular, we focus on "discrete time crystals", which are many-body phases of matter characterized by a spontaneously broken discrete time translation symmetry. We give a definition of discrete time crystals from several points of view, emphasizing that they are a non-equilibrium phenomenon, which is stabilized by many-body interactions, with no analog in non-interacting systems. We explain the theory behind several proposed models of discrete time crystals, and compare a number of recent realizations, in different experimental contexts.

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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