The energy levels of the conduction electrons in graphite, in the presence of a magnetic field, are calculated by the method of the tight binding approximation, taking into account the effect of band-to-band transitions which is not included in the Landau-Peierls treatment. The present theory is a natural extension of the Luttinger-Kohn and McClure theories for the band structure of graphite. The relation to the diamagnetic susceptibility is discussed.
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Hisanao Sato (1959) studied this question.
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