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For extended states, the integral is performed far into the semiconductor where the potential is negligible and the wave function are matched to appropriate traveling waves in the bulk semiconductor. For localized states, the integral is performed similarly far into the semiconductor and the occurrence of a localized state corresponds to the situation when the wave function obtained from the integration goes to zero (as opposed to diverging) at this large value of z.
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For extended states, the integral is performed far into the semiconductor where the potential is negligible and the wave function are matched to appropriate traveling waves in the bulk semiconductor. For localized states, the integral is performed similarly far into the semiconductor and the occurrence of a localized state corresponds to the situation when the wave function obtained from the integration goes to zero (as opposed to diverging) at this large value of z.
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