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Radiative-recoil corrections to hyperfine splitting in muonium of orders and are calculated. These corrections are of the second order in the small electron-muon mass ratio. An analytic expression $(-6 \ln2- \frac{3}{4})\alpha (Z\alpha) - \frac{17}{12} (Z^2 \alpha) (Z\alpha)^2 E_F$ is obtained. Numerically the correction is equal to and is of the same order of magnitude as the expected accuracy of the current Los Alamos experiment to measure the hyperfine splitting.

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