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Density of electron states in crystalline systems calculated in the presence and absence of the magnetic field

机译:在存在和不存在磁场的情况下计算的晶体系统中电子态的密度

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It is demonstrated in terms of explicit calculations that the average density of states in a crystalline system remains unaffected by the presence of the external magnetic field. This is so on condition the magnetic field is weak enough to provide us with a large number of the Landau levels per energy unit. For a special case of a two-dimensional crystalline system, the equivalence of the density of states obtained in the presence and the absence of the magnetic field can be shown in an analytic way. For three dimensions, the tightly bound s-electron states in crystals having cubic symmetry are taken into consideration. Here the density of states calculated in the presence of the magnetic field is compared numerically with that of the field-absent Bloch states acquired with the aid of Jelitto's method. (c) 2006 Wiley Periodicals, Inc.
机译:根据显式计算证明,晶体系统中平均态密度不受外部磁场的影响。在磁场弱到足以为我们提供大量每个能量单位的朗道能级的情况下,情况如此。对于二维晶体系统的特殊情况,可以以解析的方式示出在存在和不存在磁场的情况下获得的状态密度的等价性。对于三个维度,要考虑具有立方对称性的晶体中紧密结合的s电子态。在此,将在磁场存在下计算出的状态密度与借助Jelitto方法获得的无场布洛赫状态的密度进行数值比较。 (c)2006年Wiley Periodicals,Inc.

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