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A pool of potential energies at which defect states can be created is incorporated into a simple chemical-equilibrium description of defect formation in a-Si:H. For a wide enough defect-pool distribution, D^- lies deeper in the gap than D⁰, in agreement with recent photoemission results, even though the correlation energy is positive. Bonded hydrogen is proposed as the physical origin of the defect pool.
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K. Winer (1989) studied this question.
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