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For B = 0 the upper spin-subband density is smaller than half the p because of the inversion-asymmetry-induced spin splitting of the subband states [10].
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34
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e [B. E. Cole et al., Phys. Rev. B 55, 2503 (1997)]. In our calculations we obtain a density-of-states m* at B = 0 with approximately the same value.
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