Abstract

The changes in resistivity of silicon samples containing group III and group V impurities have been measured at hydrostatic pressures up to 6000 kg ${\mathrm{cm}}^{\ensuremath{-}2}$ at 50\ifmmode^\circ\else\textdegree\fi{}K. The changes are explained by a dependence on pressure of the ionization energy of the majority impurity center. The results indicate that the arsenic energy level moves toward the conduction-band edge at a rate of approximately 5\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}8}$ eV ${\mathrm{kg}}^{\ensuremath{-}1}$ ${\mathrm{cm}}^{2}$. The energy levels for indium and aluminum move away from the valence-band edge at rates of about 5\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}8}$ eV ${\mathrm{kg}}^{\ensuremath{-}1}$ ${\mathrm{cm}}^{2}$ and 1\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}8}$ eV ${\mathrm{kg}}^{\ensuremath{-}1}$ ${\mathrm{cm}}^{2}$, respectively. Corrections for the changes in mobility with pressure have been applied for the $n$-type sample. The motion of the arsenic energy level is explained by a change in dielectric constant and effective mass with pressure, and indicates a change in the average effective mass of less than 1% in 5000 kg ${\mathrm{cm}}^{\ensuremath{-}2}$. The very small changes in ionization energy, while expected, are to be contrasted with the much larger changes found for the deep-lying levels produced by elements such as gold.

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