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arXiv 2102.08879cond-mat.mes-hallmath-phmath.MPquant-ph
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经典和量子物理问题中轨道Angular Momentum的拓扑泡利相和分数量子化

Topological Pauli Phase and Fractional Quantization of Orbital Angular Momentum in the Problems of Classical and Quantum Physics

K. S. Krylov, V. M. Kuleshov, Yu. E. Lozovik, V. D. Mur

摘要:

在二维Helmholtz、Schroedinger和Dirac方程的框架下讨论了非平凡拓扑Pauli相(即角轨道角动量的分数量子化,这在二维情形下是可能的)的存在性所必需的物理问题.作为经典场论中的例子,我们考虑一个“楔形问题”--描述两个导电半平面之间的点电荷产生的场--和刀口的菲涅耳衍射。在少电子圆形量子点中,轨道角动量的整数和半整数量子化之间的选择由泡利原理定义。这与垂直磁场中这种量子点基态能量的精确实验数据一致。在无间隙石墨烯中,如在有间隙石墨烯的情况下,在存在过充电杂质的情况下,该问题可以通过实验解决,例如,使用扫描隧道光谱法。

英文摘要:

Physical problems for which the existence of non-trivial topological Pauli phase (i.e. fractional quantization of angular orbital angular momenta that is possible in 2D case) is essential are discussed within the framework of two-dimensional Helmholtz, Schroedinger and Dirac equations. As examples in classical field theory we consider a "wedge problem" -- a description of a field generated by a point charge between two conducting half-planes -- and a Fresnel diffraction from knife-edge. In few-electron circular quantum dots the choice between integer and half-integer quantization of orbital angular momenta is defined by the Pauli principle. This is in line with precise experimental data for the ground state energy of such quantum dots in a perpendicular magnetic field. In a gapless graphene, as in the case of gapped one, in the presence of overcharged impurity this problem can be solved experimentally, e.g., using the method of scanning tunnel spectroscopy.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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