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- W2003175761 abstract "Main consequences of the two-meson theory by Marshak and Bethe on the one hand and that by Sakata are compared with experiments concerning $ensuremath{pi}$- and $ensuremath{mu}$-mesons. It is shown that the pair type interaction between $ensuremath{pi}$-mesons and nucleons in M. B. theory contradicts with frequent occurrence of stars produced by $ensuremath{pi}$-mesons, whereas the assumption in Sakata theory that $ensuremath{pi}$-mesons with spin 0 or 1 are responsible for nuclear forces does not. Although the smaller range for the nuclear forces thus obtained from the latter theory is not at variance with the high energy neutron-proton scattering experiment, deuteron quadrupole moment cannot be accounted for by a $ensuremath{pi}$-meson field alone, so that the admixture of another meson field with larger range is necessitated. Both $ensuremath{pi}ensuremath{-}ensuremath{mu}$-decay and $ensuremath{mu}$-nuclear capture can be consistently accounted for by assuming spin textonehalf{} for $ensuremath{mu}$-mesons as in Sakata theory. However, nuclear $ensuremath{beta}$-decay and $ensuremath{mu}ensuremath{-}ensuremath{beta}$-decay have to be considered as direct processes as in Fermi's theory of $ensuremath{beta}$-decay, instead of indirect processes through virtual emission and absorption of $ensuremath{pi}$-mesons as assumed usually in the meson theory." @default.
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- W2003175761 date "1949-07-01" @default.
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- W2003175761 title "On The Two-MesonTheory1" @default.
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- W2003175761 doi "https://doi.org/10.1103/physrev.76.60" @default.
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