Eschrig M
Department of Physics, Royal Holloway, University of London, Egham, Surrey TW20 0EX, UK
Philos Trans A Math Phys Eng Sci. 2018 Aug 6;376(2125). doi: 10.1098/rsta.2015.0149.
Andreev bound states are an expression of quantum coherence between particles and holes in hybrid structures composed of superconducting and non-superconducting metallic parts. Their spectrum carries important information on the nature of the pairing, and determines the current in Josephson devices. Here, I focus on Andreev bound states in systems involving superconductors and ferromagnets with strong spin-polarization. I provide a general framework for non-local Andreev phenomena in such structures in terms of coherence functions, and show how the latter link wave function and Green-function based theories.This article is part of the theme issue 'Andreev bound states'.
安德列夫束缚态是由超导和非超导金属部分组成的混合结构中粒子与空穴之间量子相干的一种表现形式。它们的能谱携带了有关配对性质的重要信息,并决定了约瑟夫森器件中的电流。在这里,我关注涉及具有强自旋极化的超导体和铁磁体的系统中的安德列夫束缚态。我根据相干函数为这类结构中的非局域安德列夫现象提供了一个通用框架,并展示了后者如何将基于波函数和格林函数的理论联系起来。本文是主题为“安德列夫束缚态”的一部分。