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Macroscopic quantum tunneling and quantum-classical phase transitions of the escape rate in large spin systems

机译:宏观量子隧穿和量子经典相变   大型旋转系统的逃逸率

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摘要

This article presents a review on the theoretical and the experimentaldevelopments on macroscopic quantum tunneling and phase transition of theescape rate in spin systems. We present the basic ideas with simplifiedcalculations so that it is readable to both specialists and nonspecialists inthis area of research. A brief derivation of the path integral formulation ofquantum mechanics in its original form using the orthonormal position andmomentum basis is reviewed. For spin systems such as single molecule magnets,the formulation of path integral requires the use of non-orthonormal spincoherent state in $(2s+1)$ dimensional Hilbert space, the coordinateindependent and the coordinate dependent form of the spin coherent state pathintegral is derived. These two forms of spin coherent state path integral areapplied to the tunneling of single molecule magnets through its magneticanisotropy barrier. Most experimental and numerical results are presented. Thesuppression of tunneling for half-odd integer spin (spin-parity effect) at zeromagnetic field is derived from both forms, which shows that this result(spin-parity effect) is independent of the coordinate. At nonzero magneticfield we present both the experimental and the theoretical results of theoscillation of tunneling splitting as a function of the applied magnetic fieldapplied along the spin hard anisotropy axis direction. The experimental and thetheoretical results of the tunneling in antiferromagnetic exchange coupleddimer model are also reviewed. As the spin coherent state path integralformalism is a semi-classical method, an alternative exact mapping of a spinsystem to a particle in a potential field (effective potential method) isderived. This effective potential method allows for the investigation of phasetransition of the escape rate in spin systems.
机译:本文介绍了自旋系统中宏观量子隧穿和逸出速率相变的理论和实验研究进展。我们以简化的计算方式介绍了基本思想,以便该领域的专家和非专家都能阅读。回顾了使用正交位置和动量基础对量子力学原始形式的路径积分公式的简要推导。对于单分子磁体之类的自旋系统,路径积分的形成要求在$(2s + 1)$维希尔伯特空间中使用非正交自旋相干态,得出自旋相干态路径积分的坐标独立形式和坐标独立形式。这两种形式的自旋相干态路径积分被应用于单分子磁体通过其磁各向异性势垒的隧穿。给出了大多数实验和数值结果。两种形式都得出了零磁场下半奇数整数自旋的隧穿抑制(自旋奇偶效应),这表明该结果(自旋奇偶效应)与坐标无关。在非零磁场下,我们给出了隧穿分裂振荡的实验和理论结果,它们是沿着自旋硬各向异性轴方向施加的施加磁场的函数。综述了反铁磁交换耦合二聚体模型中隧穿的实验和理论结果。由于自旋相干态路径积分形式主义是一种半经典方法,因此得出了自旋系统到势场中粒子的替代精确映射(有效势方法)。这种有效的潜在方法允许研究自旋系统中逸出速率的相变。

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