Impurity Conduction in Transmutation-Doped<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>p</mml:mi></mml:math>-Type Germanium

The Hall coefficient and resistivity of germanium single crystals bombarded with slow neutrons were measured between 1.2 and 300\ifmmode^\circ\else\textdegree\fi{}K. Slow neutron capture and subsequent nuclear transmutation produce majority impurities, gallium atoms, and compensating impurities, arsenic and selenium atoms. $p$-type samples with a gallium concentration ranging from 8\ifmmode\times\else\texttimes\fi{}${10}^{14}$ to 5\ifmmode\times\else\texttimes\fi{}${10}^{17}$ per cc with a fixed compensation ratio of 0.40 were thus prepared and the impurity conduction was studied as a function of the average distance between the majority impurities. The effective radius $a$ of the acceptor ground-state wave function is 90.1 A according to Miller's theory of impurity conduction, whereas $a=40$ A according to Twose's theory. The latter value agrees well with the effective radius of the Kohn-Schechter acceptor wave function. The activation energy of impurity conduction changes slowly with impurity concentration from 3.5\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}4}$ to 5.9\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}4}$ ev and agrees well with the predictions of Miller's theory for gallium concentration below 5\ifmmode\times\else\texttimes\fi{}${10}^{15}$ per cc. Measurements on samples which contain different dislocation densities but identical impurity concentrations show that up to ${10}^{4}$ dislocations per ${\mathrm{cm}}^{2}$ do not affect impurity conduction.

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