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They behave as amorphous semiconductors.
The first electronic application of amorphous semiconductors to occur on a large scale was in xerography (or electrostatic imaging), the process that provides the basis of plain-paper copiers.
Amorphous semiconductors, in the form of thin films prepared by methods such as that shown in Figure 4D, are important in applications requiring large areas of electronically active material.
Mostly, the fundamental absorption edge observed in amorphous semiconductors follows an exponential law.
A class of nanomaterials that display these characteristics is amorphous semiconductors [1].
In the case of amorphous semiconductors, the fundamental absorption edge follows an exponential law.
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A related end-member of this group is the elemental amorphous semiconductor solids, such as amorphous silicon (a-Si) and amorphous germanium (a-Ge).
This important amorphous semiconductor is also used as the image sensor in facsimile ("fax") machines, and it serves as the photoreceptor in some xerographic copiers.
As shown in the table of technological applications of amorphous solids, the practical form of this amorphous semiconductor is not pure silicon but a silicon-hydrogen alloy containing 10 percent hydrogen.
A new equivalent circuit has been assumed, based on recent theory of an amorphous semiconductor Schottky barrier.
In disordered materials, such as amorphous semiconductor or some thin films, low temperature transport occurs between localized electronic states near the Fermi level (EF).
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