1982
DOI: 10.1103/physrevb.25.2776
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Impurity-band density of states in heavily doped semiconductors: Numerical results

Abstract: The "band-tail" density of states p(E) available to electrons in a field of randomly distributed, attractive impurities developed in previous work is extended to higher energy E. Numerical values of p(E) are also presented (1) for comparison with p(E) developed by other methods and (2) for calculation of optical and other properties of heavily doped semicoflductors depending on p(E).

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Cited by 21 publications
(8 citation statements)
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“…WðXðsÞ À XðrÞÞ ¼ ð dx VðXðsÞ À xÞ VðXðrÞ À xÞ: (2) An electron moving in a field of random impurities can be described by the action 1…”
mentioning
confidence: 99%
“…WðXðsÞ À XðrÞÞ ¼ ð dx VðXðsÞ À xÞ VðXðrÞ À xÞ: (2) An electron moving in a field of random impurities can be described by the action 1…”
mentioning
confidence: 99%
“…(B.5): Δr ≫ 0 as → −0. Finally, we also remark that, in the full ground-state case and deep-tail approximation, the exponential conduction-band tail, obtained by Sa-yakamit et al [23], was also equal to a constant at = −0, being not correct.…”
Section: Feynman Path-integral Methodsmentioning
confidence: 65%
“…Therefore, the density of states, the optical absorption coefficient and the electrical conductivity, being proportional to our result (20), vanished at the conduction-band edge = 0, as given in Eqs. (23,26). Those results were also compared with other theoretical results, obtained at − = 0, in the small time approximation [21,29,30] and in the full ground-state case and deep-tail approximation [21], which were found to be constant, being not correct, as discussed also in Eq.…”
Section: Introductionmentioning
confidence: 75%
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