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x predicted by the band-anticrossing (BAC) model. However, we estimate that the nonparabolicity introduced by the BAC interaction between the CB states of InAs and the N-levels would reduce our values of εth by less than 1%. This correction is obtained by fitting the energy dispersions from the BAC model with the nonparabolic dispersions of Ref. using as fitting parameter the nonparabolicity factor α. The fitting provides a good description of the energy dispersions over an extended energy range, i.e., from 0 to 0.7 eV.
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