Band-tail states are routinely invoked in models of a-Si:H, including defect pool models and models of light-induced defects. These models describe the band-tail states as being localized on a single stretched bond. However, to our knowledge, there is no theoretical or experimental work to justify these assumptions. In this work we use ab initio calculations to support earlier tight-binding calculations that show that the band-tail states are very delocalized---involving large numbers of atoms as the energy is varied from midgap into the tails. Our work also shows that valence-band-tail states are statistically associated with short bonds (not long bonds), and conduction-band states with long bonds. We have slightly modified a 512-atom model of a-Si due to Djordjevic, Thorpe, and Wooten [Phys. Rev. B 52, 5688 (1995)] to produce a large model of a-Si:H with realistic band tails, radial distribution function, and vibrational spectrum. Above all, we created and used a model with no spectral or geometrical defects.
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Fedders et al. (1998) studied this question.