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Role of spin degrees of freedom in Anderson localization of two-dimensional particle gases with random spin-orbit interactions

机译:自旋自由度在具有随机自旋轨道相互作用的二维粒子气体的安德森局部化中的作用

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摘要

Anderson localization of two-dimensional noninteracting high-spin particle gases subject to random spin-orbit coupling and random on-site potential is numerically studied on square lattices. Employing the finite-size scaling of localization length, we show that the Anderson localization transition occurs for high-spin fermions and belongs to the same universality class as two-dimensional systems with time-reversal symmetry and spin-orbit interaction characterized by the universal critical exponent of nu similar or equal to 2.73, while all states of disordered bosons are localized in the thermodynamic limit. These observations are commensurate with the scaling theory. Moreover, a strong finite-size effect is observed for high-spin particles, which can be attributed to the large spin degrees of freedom acting as an extra spin dimension in finite lattices. As a consequence, the system indeed behaves as a three-dimensional system and the Anderson localization transition can even happen for bosons with very large spins when the spin degrees of freedom is comparable to the lattice size.
机译:在方格上数值研究了二维非相互作用高自旋粒子气体在随机自旋-轨道耦合和随机现场势的作用下的安德森局部化。利用局域长度的有限尺寸定标,我们证明了安德森局域性转变发生在高自旋费米子上,并且与具有时间反转对称性和自旋轨道相互作用的二维系统具有相同的普遍性,其特征是普遍临界nu的指数相似或等于2.73,而无序玻色子的所有状态都位于热力学极限内。这些观察结果与定标理论相称。此外,对于高自旋粒子,观察到了很强的有限尺寸效应,这可以归因于较大的自旋自由度在有限晶格中充当额外的自旋尺寸。结果,该系统确实表现为三维系统,并且当自旋自由度与晶格大小相当时,甚至对于自旋非常大的玻色子也可能发生安德森局部化转变。

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