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中国物理学会期刊

宇称-时间对称与反对称研究进展

CSTR: 32037.14.aps.71.20221323

Research progress of parity-time symmetry and anti-symmetry

CSTR: 32037.14.aps.71.20221323
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  • 在标准量子力学中, 描述物理系统的哈密顿量一般是厄米的,以保证系统具有实能谱及系统演化的幺正性. 近些年来, 研究发现具有宇称-时间(parity-time, \cal PT )对称特性的非厄米哈密顿量也具有实能谱, 并且在\cal PT 对称相和\cal PT 对称破缺相之间存在一个新奇的非厄米奇异点, 这是厄米系统所不具有的. 最近, 人们在各种各样的物理系统中实现了\cal PT 对称和\cal PT 反对称的非厄米哈密顿量, 并演示了新奇的量子现象, 这不仅加深了对基本量子物理规律的理解, 也促进了应用技术的突破. 本综述将介绍\cal PT 对称和\cal PT 反对称的基本物理原理, 总结在光学系统和原子系统中实现\cal PT 对称和\cal PT 反对称的方案, 并回顾利用\cal PT 对称系统非厄米奇异点进行精密传感的研究.

     

    In standard quantum mechanics, the Hamiltonian describing the physical system is generally Hermitian, so as to ensure that the system has real energy spectra and that the system’s evolution is unitary. In recent years, it has been found that non-Hermitian Hamiltonians with parity-time (\cal PT) symmetry also have real energy spectra, and there is a novel non-Hermitian exceptional point between \cal PT-symmetric phase and \cal PT -symmetry-broken phase, which is unique to non-Hermitian systems. Recently, people have realized \cal PT symmetric and anti-\cal PT symmetric non-Hermitian Hamiltonians in various physical systems and demonstrated novel quantum phenomena, which not only deepened our understanding of the basic laws of quantum physics, but also promoted the breakthrough of application technology. This review will introduce the basic physical principles of \cal PT symmetry and anti-\cal PT symmetry, summarize the schemes to realize \cal PT symmetry and anti-\cal PT symmetry in optical and atomic systems systematically, including the observation of \cal PT -symmetry transitions by engineering time-periodic dissipation and coupling in ultracold atoms and single trapped ion, the realization of anti-\cal PT symmetry in dissipative optical system by indirect coupling, and realizing anti-\cal PT -symmetry through fast atomic coherent transmission in flying atoms. Finally, we review the research on precision sensing using non-Hermitian exceptional points of \cal PT -symmetric systems. Near the exceptional points, the eigenfrequency splitting follows an \varepsilon ^\tfrac1N-dependence, where the \varepsilon is the perturbation and N is the order of the exceptional point. We review the \cal PT-symmetric system composed of three equidistant micro-ring cavities and enhanced sensitivity at third-order exceptional points. In addition, we also review the debate on whether exceptional-point sensors can improve the signal-to-noise ratio when considering noise, and the current development of exceptional-point sensors, which is still an open and challenging question.

     

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