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磁性分子簇中的量子相位干涉和宇称效应。

Quantum phase interference and parity effects in magnetic molecular clusters.

作者信息

Wernsdorfer W, Sessoli R

机构信息

Laboratoire Louis Neel, CNRS, BP166, 38042 Grenoble, France. Department of Chemistry, University of Florence, Via Maragliano 75/77, 50144 Firenze, Italy.

出版信息

Science. 1999 Apr 2;284(5411):133-5. doi: 10.1126/science.284.5411.133.

Abstract

An experimental method based on the Landau-Zener model was developed to measure very small tunnel splittings in molecular clusters of eight iron atoms, which at low temperature behave like a nanomagnet with a spin ground state of S = 10. The observed oscillations of the tunnel splittings as a function of the magnetic field applied along the hard anisotropy axis are due to topological quantum interference of two tunnel paths of opposite windings. Transitions between quantum numbers M = -S and (S - n), with n even or odd, revealed a parity effect that is analogous to the suppression of tunneling predicted for half-integer spins. This observation is direct evidence of the topological part of the quantum spin phase (Berry phase) in a magnetic system.

摘要

一种基于朗道-齐纳模型的实验方法被开发出来,用于测量八个铁原子分子簇中非常小的隧道分裂,这些分子簇在低温下表现得像一个自旋基态为S = 10的纳米磁体。观察到的隧道分裂随沿硬各向异性轴施加的磁场的振荡是由于两个相反缠绕的隧道路径的拓扑量子干涉。量子数M = -S和(S - n)(n为偶数或奇数)之间的跃迁揭示了一种宇称效应,该效应类似于对半整数自旋预测的隧道效应抑制。这一观察结果是磁系统中量子自旋相(贝里相)拓扑部分的直接证据。

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