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The disorder characteristic of amorphous semiconductors introduces tails of states which encroach upon the otherwise empty gap region
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The disorder characteristic of amorphous semiconductors introduces tails of states which encroach upon the otherwise empty gap region.
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Cody et al. (Ref. 8) provided evidence in support of this "universal" relationship for the case of hydrogenated amorphous silicon. Persans et al. (Ref. 10) provided evidence in support of this "universal" relationship for the case of hydrogenated amorphous germanium
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Cody et al. (Ref. 8) provided evidence in support of this "universal" relationship for the case of hydrogenated amorphous silicon. Persans et al. (Ref. 10) provided evidence in support of this "universal" relationship for the case of hydrogenated amorphous germanium.
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Jackson et al. (Ref. 15) provide experimental evidence which suggests that the JDOS function dominates the optical absorption spectrum of hydrogenated amorphous silicon
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Jackson et al. (Ref. 15) provide experimental evidence which suggests that the JDOS function dominates the optical absorption spectrum of hydrogenated amorphous silicon.
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Owing to the fact that our semiclassical approach neglects quantum confinement effects, our model is not applicable to physical systems with large and abrupt potential fluctuations, such as those which occur in hydrogenated amorphous silicon nitride (Ref. 18) and amorphous carbon (Ref. 17)
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Owing to the fact that our semiclassical approach neglects quantum confinement effects, our model is not applicable to physical systems with large and abrupt potential fluctuations, such as those which occur in hydrogenated amorphous silicon nitride (Ref. 18) and amorphous carbon (Ref. 17).
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0010504024
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The normalized JDOS function is proportional to J(ω) and is as defined in Ref. 6
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The normalized JDOS function is proportional to J(ω) and is as defined in Ref. 6.
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