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The changes in resistivity of silicon samples containing gold impurity, which are appropriately counterdoped with hydrogenic impurities, have been measured at hydrostatic pressures up to 30 000 kg cm^-2 near room temperature. The changes are explained by a dependence on pressure of the ionization energy of the gold impurity.The pressure coefficient of the energy of a gold acceptor level near the center of the forbidden gap has been determined, relative to both band edges; the coefficient of the separation from the conduction band edge is twice that of the separation from the valence band. The sum of the two coefficients gives a pressure coefficient for the total energy gap of -1.5×{}10^-6 eV kg^-1 cm² between 0 and 4000 kg cm^-2 or -2.4×{}10^-6 eV kg^-1 cm² near 20 000 kg cm^-2. The low-pressure value is in agreement with previous, more direct, determinations. A donor level due to the gold, roughly 0.35 eV above the valence band edge, has a very low pressure coefficient relative to that edge.
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Nathan et al. (1962) studied this question.
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