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关联纳米尺度系统中的Levitons

Levitons in correlated nano-scale systems.

作者信息

Ronetti F, Bertin-Johannet B, Popoff A, Rech J, Jonckheere T, Grémaud B, Raymond L, Martin T

机构信息

Aix Marseille Univ, Université de Toulon, CNRS, CPT, IPhU, AMUTECH, Marseille, France.

出版信息

Chaos. 2024 Apr 1;34(4). doi: 10.1063/5.0199567.

DOI:10.1063/5.0199567
PMID:38668587
Abstract

In this short review (written to celebrate David Campbell's 80th birthday), we provide a theoretical description of quantum transport in nanoscale systems in the presence of single-electron excitations generated by Lorentzian voltage drives, termed Levitons. These excitations allow us to realize the analog of quantum optics experiments using electrons instead of photons. Importantly, electrons in condensed matter systems are strongly affected by the presence of different types of non-trivial correlations, with no counterpart in the domain of photonic quantum optics. After providing a short introduction about Levitons in non-interacting systems, we focus on how they operate in the presence of two types of strong electronic correlations in nanoscale systems, such as those arising in the fractional quantum Hall effect or in superconducting systems. Specifically, we consider Levitons in a quantum Hall bar of the fractional quantum Hall effect, pinched by a quantum point contact, where anyons with fractional charge and statistics tunnel between opposite edges. In this case, a Leviton-Leviton interaction can be induced by the strongly correlated background. Concerning the effect of superconducting correlations on Levitons, we show that, in a normal metal system coupled to BCS superconductors, half-integer Levitons minimize the excess noise in the Andreev regime. Interestingly, energy-entangled electron states can be realized on-demand in this type of hybrid setup by exploiting crossed Andreev reflection. The results exposed in this review have potential applications in the context of quantum information and computation with single-electron flying qubits.

摘要

在这篇简短的综述(为庆祝大卫·坎贝尔80岁生日而撰写)中,我们给出了在存在由洛伦兹电压驱动产生的单电子激发(称为莱维顿)的情况下,纳米尺度系统中量子输运的理论描述。这些激发使我们能够利用电子而非光子来实现量子光学实验的类似物。重要的是,凝聚态物质系统中的电子受到不同类型非平凡关联的强烈影响,这在光子量子光学领域中并无对应情况。在对非相互作用系统中的莱维顿进行简短介绍之后,我们聚焦于它们在纳米尺度系统中两种强电子关联存在时的运作方式,比如在分数量子霍尔效应或超导系统中出现的那些关联。具体而言,我们考虑在分数量子霍尔效应的量子霍尔条中,由量子点接触夹住的莱维顿,其中具有分数电荷和统计特性的任意子在相对边缘之间隧穿。在这种情况下,莱维顿 - 莱维顿相互作用可由强关联背景诱导产生。关于超导关联对莱维顿的影响,我们表明,在与BCS超导体耦合的正常金属系统中,半整数莱维顿在安德列夫区域使过量噪声最小化。有趣的是,通过利用交叉安德列夫反射,在这种混合装置中可以按需实现能量纠缠的电子态。本综述中揭示的结果在利用单电子飞行量子比特进行量子信息和计算方面具有潜在应用。

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