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arXiv 1610.09752quant-phcond-mat.stat-mech
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非厄米相变的普适临界行为

Universal Critical Behaviors in Non-Hermitian Phase Transitions

Bo-Bo Wei, Liang Jin

摘要:

量子相变也发生在非厄米系统中。在这项工作中,我们表明,密度泛函理论,第一次,揭示了非厄米多体系统的相变的普遍行为。具体地说,我们首先证明了非厄米量子多体系统的非简并定态是定态能量对控制参数的一阶导数的普适函数。这一发现对非厄米特系统具有深远的影响:(i)它将物理可观测的非解析行为和稳态能量的非解析行为联系起来,这解释了为什么非厄米特系统中的量子相变发生在有限系统中。(ii)它预言了任何物理观测在非厄米相变点的普遍标度行为,标度指数为$(1-1/p),2(1-1/p),\cdots,n(1-1/p),\cdots$,其中$p$为例外点处的合并态数,$n$为正整数.(iii)。结果表明,在非厄米相变点处,量子纠缠呈现出普适的标度行为,临界指数为$(1-1/p),2(1-1/p),\cdots,n(1-1/p),\cdots$ .这些结果揭示了非厄米相变的普遍临界行为,提供了非厄米量子多体物理中纠缠与相变之间的深刻联系,为非厄米系统的量子精密测量奠定了基础.

英文摘要:

Quantum phase transitions also occur in non-Hermitian systems. In this work we show that density functional theory, for the first time, uncovers universal behaviors for phase transitions in non-Hermitian many-body systems. To be specific, we first prove that the non-degenerate steady state of a non-Hermitian quantum many-body system is a universal function of the first derivative of the steady state energy with respect to the control parameter. This finding has far-reaching consequences for non-Hermitian systems: (i) It bridges the nonanalytic behavior in physical observable and nonanalytic behavior of steady state energy, which explains why the quantum phase transitions in non-Hermitian systems occur for finite systems. (ii) It predicts universal scaling behaviors of any physical observable at non-Hermitian phase transition point with scaling exponent being $(1-1/p),2(1-1/p),\cdots,n(1-1/p),\cdots$ with $p$ being the number of coalesced states at the exceptional point and $n$ being a positive integer. (iii). It reveals that quantum entanglement in non-Hermitian phase transition point presents universal scaling behaviors with critical exponents being $(1-1/p),2(1-1/p),\cdots,n(1-1/p),\cdots$. These results uncover universal critical behaviors in non-Hermitian phase transitions and provide profound connections between entanglement and phase transition in non-Hermitian quantum many-body physics and establish foundations for quantum metrology in non-Hermitian systems.

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