Abstract

The hyperfine splitting of muonium in Si and Ge is analyzed on various models of the dielectric properties of the medium. Muonium acts as a deep donor in Si and Ge, contrary to some earlier predictions. It is possible to give a reasonable account of the observed values of ${|\ensuremath{\psi}(0)|}^{2}$ in terms of the Reiss-Kaus cavity models, and in terms of the Walter-Cohen $\ensuremath{\epsilon}(q)$ calculated from the actual band structures, provided that the electron mass is taken as essentially equal to the free-electron mass. Identical results are expected for interstitial atomic hydrogen.

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