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The symmetry of three-electron states in a quantized magnetic field

机译:量子磁场中三电子态的对称性

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The states of itinerant electrons on the finite square lattice in a quantized magnetic field are discussed. The single-electron states are classified by irreducible representations (IRs) of the magnetic translation group.The representation correspond to the Landau level, whereas its basis functions are analogs of the cyclotronic orbits. The filling factor of the Landau level is considered in the frame of multi-electron functions. Corresponding states are classified by the IR of MTG as well as by the irreducible representation of a symmetric group (permuting the electrons) and a unitary group (permuting electron states). The discussion is restricted to the case when the magnetic flux per unit cell of the two-dimensional square lattice is a rational number in terms of magnetic flux quanta. The additional parameter of the model is the Hubbard interaction between electrons.
机译:讨论了在有限磁场中有限正方形晶格上流动电子的状态。单电子态通过磁平移群的不可约表示(IR)进行分类,该表示对应于Landau能级,而其基本函数是回旋轨道的类似物。在多电子功能的框架内考虑了朗道能级的填充因子。相应的状态通过MTG的IR以及对称基团(置换电子)和a基团(置换电子态)的不可约表示进行分类。讨论限于二维方格子的每单位晶胞的磁通量在磁通量方面是有理数的情况。该模型的附加参数是电子之间的Hubbard相互作用。

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