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 |ψ(0)|² in terms of the Reiss-Kaus cavity models, and in terms of the Walter-Cohen ε(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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Wang et al. (1973) studied this question.
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