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Observation of the two-channel Kondo effect

机译:观察两通道近藤效应

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摘要

Some of the most intriguing problems in solid-state physics arise when the motion of one electron dramatically affects the motion of surrounding electrons. Traditionally, such highly correlated electron systems have been studied mainly in materials with complex transition metal chemistry. Over the past decade, researchers have learned to confine one or a few electrons within a nanometre-scale semiconductor 'artificial atom', and to understand and control this simple system in detail. Here we combine artificial atoms to create a highly correlated electron system within a nano-engineered semiconductor structure. We tune the system in situ through a quantum phase transition between two distinct states, each a version of the Kondo state, in which a bound electron interacts with surrounding morale electrons. The boundary between these competing Kondo states is a quantum critical point—namely, the exotic and previously elusive two-channel Kondo state, in which electrons in two reservoirs are entangled through their interaction with a single localized spin.
机译:当一个电子的运动极大地影响周围电子的运动时,就会出现一些固态物理学中最令人着迷的问题。传统上,主要在具有复杂过渡金属化学的材料中研究这种高度相关的电子系统。在过去的十年中,研究人员学会了将一个或几个电子限制在纳米级半导体“人造原子”中,并详细了解和控制这个简单的系统。在这里,我们将人造原子结合在一起,在纳米工程半导体结构内创建高度相关的电子系统。我们通过两个不同状态之间的量子相变来原位调整系统,每个状态都是近藤状态的一种,其中束缚电子与周围的士气电子相互作用。这些竞争的近藤状态之间的边界是一个量子临界点,即奇异的,以前难以捉摸的两通道近藤状态,其中两个储层中的电子通过与单个局部自旋的相互作用而纠缠在一起。

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