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Quantum-dynamical phase transition and Fisher information in a non-Hermitian Bose-Hubbard dimer

机译:非Hermitian Bose-Hubbard二聚体中的量子动力学相变和Fisher信息

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We study the dynamical properties in a non-Hermitian Bose-Hubbard dimer and show that the steady state consists mostly of the eigenstate whose eigenvalue has the largest imaginary part. A sharp phase transition occurs in the steady state and the phase transition occurs for a finite particle number, not for infinite ones, in contrast to the Hermitian system. We also investigate the quantum Fisher information and entanglement in two different phases. The results show that the steady state in the Josephson oscillation regime is fully N-particle entangled and the corresponding parameter sensitivity approaches the Heisenberg limit. In the self-trapping regime, the parameter sensitivity just scales as the shot-noise limit. Moreover, quantum Fisher information of the steady state is robust to the initial state, which indicates that the non-Hermitian dynamics takes more advantage than the Hermitian one for quantum metrology. Copyright (C) EPLA, 2016
机译:我们研究了非Hermitian Bose-Hubbard二聚体的动力学性质,并表明稳态主要由特征值最大虚部的本征态组成。与Hermitian系统相反,在稳态下会发生急剧的相变,并且相变发生在有限数量的粒子上,而不是无限数量的粒子上。我们还研究了两个不同阶段的量子Fisher信息和纠缠。结果表明,约瑟夫森振动状态下的稳态状态完全被N粒子纠缠,相应的参数灵敏度接近海森堡极限。在自陷机制中,参数灵敏度仅按散粒噪声极限缩放。此外,稳态的量子Fisher信息对初始状态具有鲁棒性,这表明对于量子计量学,非Hermitian动力学比Hermitian动力学更具优势。版权(C)EPLA,2016年

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