We study the magnetic field dependence of muonium–antimuonium conversion induced by neutral (pseudo)scalar bosons. Only the operator contributes to the conversion of polarized muonium, but it gets quenched by a magnetic field of strength 0.1 Gauss or stronger. Conversion induced by couplings for unpolarized muonium is independent of magnetic field. Magnetic fields of 0.1 Tesla or stronger starts to suppress conversion induced by interactions in the lowest Breit-Rabi level, but gets partially compensated by a rise in conversion probability in the other unpolarized level. The effects of $(S\mp P)(S\mp P)(S\mp P)(S\pm P)(V\mp A)(V\mp A)(V\mp A)(V\pm A)$ operators, respectively.

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