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Numerical calculations for an incommensurate phase in the Peierls instability are carried out at zero temperature by taking account of a sufficiently large number of electronic states coupled by the potential of the lattice displacement and by treating the effect of third and fifth harmonics self-consistently. Total energy of the system, amplitudes of harmonies and the pattern of the lattice displacement are calculated by changing the deviation from half-occupancy of the conduction band. The effect of harmonics is found to be essentially important in the close neighbor-hood of the half-filled case. The results extrapolated to the half-filled case are satisfactorily consistent with our analytic calculations in a preceding paper.
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Akio Kotani (1977) studied this question.
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