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有限温度下的激子极化激元约瑟夫森结。

Exciton-polariton Josephson junctions at finite temperatures.

机构信息

ITMO University, St. Petersburg, 197101, Russia.

Department of Photonics, National Chiao Tung University, Hsinchu, 300, Taiwan.

出版信息

Sci Rep. 2017 Aug 25;7(1):9515. doi: 10.1038/s41598-017-09824-8.

Abstract

We consider finite temperature effects in a non-standard Bose-Hubbard model for an exciton- polariton Josephson junction (JJ) that is characterised by complicated potential energy landscapes (PEL) consisting of sets of barriers and wells. We show that the transition between thermal activation (classical) and tunneling (quantum) regimes exhibits universal features of the first and second order phase transition (PT) depending on the PEL for two polariton condensates that might be described as transition from the thermal to the quantum annealing regime. In the presence of dissipation the relative phase of two condensates exhibits non-equilibrium PT from the quantum regime characterized by efficient tunneling of polaritons to the regime of permanent Josephson or Rabi oscillations, where the tunneling is suppressed, respectively. This analysis paves the way for the application of coupled polariton condensates for the realisation of a quantum annealing algorithm in presently experimentally accessible semiconductor microcavities possessing high (10 and more) Q-factors.

摘要

我们考虑了激子-极化激元约瑟夫森结(JJ)的非标准玻色-哈伯德模型中的有限温度效应,该模型的特点是由一系列势垒和势阱组成的复杂势能景观(PEL)。我们表明,热激活(经典)和隧道(量子)两种极化激元凝聚态之间的转变表现出第一和第二顺序相变(PT)的普遍特征,具体取决于可能被描述为从热到量子退火状态的转变的两个凝聚态的 PEL。在存在耗散的情况下,两个凝聚体的相对相位表现出非平衡 PT,从量子状态(极化激子的有效隧道)到约瑟夫森或拉比振荡的永久状态,隧道分别被抑制。这种分析为在目前实验上可达到的具有高(10 及以上)Q 因子的半导体微腔中实现量子退火算法的耦合极化激元凝聚态的应用铺平了道路。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/4e6e/5572052/7a60af515a05/41598_2017_9824_Fig1_HTML.jpg

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