It is shown that in the absence of central cell corrections, anisotropy of the donor envelope functions is the most important factor in determining the change in the metal-insulator transition density as a function of uniaxial stress in n-doped many-valley semiconductors. Quantitative agreement is obtained with experimental results for antimony-doped germanium, and a prediction made for the corresponding case in silicon.
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R. N. Bhatt (1981) studied this question.
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