Zusammenfassung
In den vorhergehenden Kapiteln haben wir gesehen, daß ein beweglicher Ladungsträger im Halbleiter eine effektive Masse m hat, die von der freien Elektronenmasse mo verschieden ist. Die effektive Masse berücksichtigt, daß der Ladungsträger einem Kristallfeld ausgesetzt ist.
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Seeger, K. (1992). Ladungs- und Wärmetransport im nichtentarteten Elektronengas. In: Halbleiterphysik. Vieweg+Teubner Verlag, Wiesbaden. https://doi.org/10.1007/978-3-322-98553-8_4
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