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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:随机旋转轨道相互作用自旋自由度旋转自由度的作用

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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 ν ? 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:二维非相互作用高自旋粒子气体经受随机自旋 - 轨道耦合和随机现场潜在的安德森本地化数值研究上正方形晶格。采用局域长度的有限尺寸缩放,我们表明,安德森本地化转变发生于高自旋费米子和属于相同的普遍性类与时间反转对称性和自旋 - 轨道相互作用的二维系统,其特征在于所述通用临界ν的指数? 2.73,而无序玻色子所有国家的热力学极限是局部的。这些观察结果与标度理论相符。另外,强大的有限尺寸效应观察到高自旋粒子,这可以归因于大的自旋自由度的作用如在有限晶格一个额外的自旋尺寸。因此,该系统的确表现为一个三维系统和安德森本地化转变,甚至可能发生了非常大的自旋玻色子当自旋自由度是相当的晶格尺寸。

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