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By combining several volume percent of conducting particles in a semicrystalline matrix, a highly temperature-dependent resistivity is obtained. The resistivity changes by several orders of magnitude in a small temperature interval centered on the crystal melting temperature. Moreover, a typical resistivity changes by a factor of hundreds as the frequency changes from 102 to 104 Hz. Materials of this type show dielectric constants in excess of 103 which vary strongly with temperature and frequency.
F. Bueche (Mon,) studied this question.
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