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全息术中的强耦合𝒫𝒯对称模型

Strongly Coupled 𝒫𝒯-Symmetric Models in Holography.

作者信息

Areán Daniel, Garcia-Fariña David, Landsteiner Karl

机构信息

Instituto de Física Teórica UAM/CSIC, Campus de Cantoblanco, c/Nicolás Cabrera 13-15, 28049 Madrid, Spain.

Departamento de Física Teórica, Universidad Autónoma de Madrid, Campus de Cantoblanco, 28049 Madrid, Spain.

出版信息

Entropy (Basel). 2024 Dec 27;27(1):13. doi: 10.3390/e27010013.

Abstract

Non-Hermitian quantum field theories are a promising tool to study open quantum systems. These theories preserve unitarity if PT symmetry is respected, and in that case, an equivalent Hermitian description exists via the so-called Dyson map. Generically, PT-symmetric non-Hermitian theories can also feature phases where PT symmetry is broken and unitarity is lost. We review the construction of holographic duals to strongly coupled PT-symmetric quantum field theories and the study of their phase diagram. We next focus on spacetime-dependent non-Hermitian couplings: non-Hermitian quenches and lattices. They violate the null energy condition in the gravity dual. The lattices realize phases supporting an imaginary current that breaks PT symmetry spontaneously. Remarkably, these non-Hermitian lattices flow to a PT-symmetric fixed point in the IR.

摘要

非厄米量子场论是研究开放量子系统的一种很有前景的工具。如果PT对称性得到尊重,这些理论会保持幺正性,在这种情况下,通过所谓的戴森映射存在一个等效的厄米描述。一般来说,PT对称的非厄米理论也可能具有PT对称性被破坏且幺正性丧失的相。我们回顾了强耦合PT对称量子场论的全息对偶的构建及其相图的研究。接下来,我们关注依赖于时空的非厄米耦合:非厄米猝灭和晶格。它们在引力对偶中违反了零能量条件。晶格实现了支持自发破坏PT对称性的虚电流的相。值得注意的是,这些非厄米晶格在红外区域流向一个PT对称的不动点。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b06/11764355/eced7b1c0fda/entropy-27-00013-g001.jpg

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