相互作用、多重激发系统中的量子态转移

Alexander Yue, Rubem Mondaini, Qiujiang Guo, Richard T. Scalettar
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摘要

量子态传输(QST)描述了量子信息从网络中的一个节点到另一个节点的相干传递。有关 QST 的实验跨越了一系列不同的平台,目前的报告显示,在几百纳秒的时间内,量子态传输跨越了多达几十个节点,保真度接近 90% 或更高。理论研究既研究了与给定(赫米特)晶格哈密顿相关的无损耗时间演化,也研究了基于允许损耗的主方程的方法。在本文中,我们介绍了蒙特卡洛技术,该技术能够发现一种能够提供高保真 QST 的哈密顿方程。我们在适合耦合光腔-发射器阵列的几何结构中对我们的方法进行了基准测试,并讨论了与传导带耦合的局部轨道的凝聚态哈密顿方程的联系。由此得出的杰恩斯-康明斯-哈伯德模型和周期性安德森模型原则上可以在适当的硬件中设计,以提供高效的 QST。
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Quantum State Transfer in Interacting, Multiple-Excitation Systems
Quantum state transfer (QST) describes the coherent passage of quantum information from one node in a network to another. Experiments on QST span a diverse set of platforms and currently report transport across up to tens of nodes in times of several hundred nanoseconds with fidelities that can approach 90% or more. Theoretical studies examine both the lossless time evolution associated with a given (Hermitian) lattice Hamiltonian and methods based on the master equation that allows for losses. In this paper, we describe Monte Carlo techniques which enable the discovery of a Hamiltonian that gives high-fidelity QST. We benchmark our approach in geometries appropriate to coupled optical cavity-emitter arrays and discuss connections to condensed matter Hamiltonians of localized orbitals coupled to conduction bands. The resulting Jaynes-Cummings-Hubbard and periodic Anderson models can, in principle, be engineered in appropriate hardware to give efficient QST.
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