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基于非厄米晶格动力学的指数增强量子传感

Exponentially-enhanced quantum sensing with non-Hermitian lattice dynamics.

作者信息

McDonald Alexander, Clerk Aashish A

机构信息

Pritzker School of Molecular Engineering, University of Chicago, Chicago, IL, 60637, USA.

Department of Physics, University of Chicago, Chicago, IL, 60637, USA.

出版信息

Nat Commun. 2020 Oct 23;11(1):5382. doi: 10.1038/s41467-020-19090-4.

DOI:10.1038/s41467-020-19090-4
PMID:33097707
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7585448/
Abstract

Non-Hermitian systems exhibit markedly different phenomena than their conventional Hermitian counterparts. Several such features, such as the non-Hermitian skin effect, are only present in spatially extended systems. Potential applications of these effects in many-mode systems however remains largely unexplored. Here, we study how unique features of non-Hermitian lattice systems can be harnessed to improve Hamiltonian parameter estimation in a fully quantum setting. While the quintessential non-Hermitian skin effect does not provide any distinct advantage, alternate effects yield dramatic enhancements. We show that certain asymmetric non-Hermitian tight-binding models with a [Formula: see text] symmetry yield a pronounced sensing advantage: the quantum Fisher information per photon increases exponentially with system size. We find that these advantages persist in regimes where non-Markovian and non-perturbative effects become important. Our setup is directly compatible with a variety of quantum optical and superconducting circuit platforms, and already yields strong enhancements with as few as three lattice sites.

摘要

非厄米系统表现出与传统厄米系统截然不同的现象。若干此类特征,比如非厄米趋肤效应,仅出现在空间扩展系统中。然而,这些效应在多模系统中的潜在应用在很大程度上仍未得到探索。在此,我们研究如何利用非厄米晶格系统的独特特征,在全量子环境中改进哈密顿量参数估计。虽然典型的非厄米趋肤效应并未提供任何明显优势,但其他效应却能带来显著增强。我们表明,某些具有[公式:见正文]对称性的非对称非厄米紧束缚模型具有明显的传感优势:每个光子的量子费舍尔信息随系统规模呈指数增长。我们发现,这些优势在非马尔可夫和非微扰效应变得重要的情况下依然存在。我们的设置与多种量子光学和超导电路平台直接兼容,并且仅需三个晶格位点就能产生强大的增强效果。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/3c4b23db7a98/41467_2020_19090_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/20849cbf2a03/41467_2020_19090_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/877f9a4f9410/41467_2020_19090_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/5cf30a4ae5d1/41467_2020_19090_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/3c4b23db7a98/41467_2020_19090_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/20849cbf2a03/41467_2020_19090_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/877f9a4f9410/41467_2020_19090_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/5cf30a4ae5d1/41467_2020_19090_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4ad4/7585448/3c4b23db7a98/41467_2020_19090_Fig4_HTML.jpg

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