We apply the Cartan’s supersymmetric model to the weak interaction of hadrons. The electromagnetic currents are transformed by G12, G123, G13, G132 and the factor(1-γ5)\documentclass[12pt]{minimal}
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\begin{document}$${(1-\gamma_5)}$$\end{document} is inserted between lν¯\documentclass[12pt]{minimal}
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\begin{document}$${l \bar\nu}$$\end{document} or l¯ν\documentclass[12pt]{minimal}
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\begin{document}$${\bar l \nu}$$\end{document} when the photon is replaced by W±\documentclass[12pt]{minimal}
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\begin{document}$${W^\pm}$$\end{document}, and between ll¯\documentclass[12pt]{minimal}
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\begin{document}$${l \bar l}$$\end{document} or νν¯\documentclass[12pt]{minimal}
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\begin{document}$${\nu\bar \nu}$$\end{document} when the photon is replaced by Z. Electromagnetic currents in the Higgs boson H0 decay into 2γ\documentclass[12pt]{minimal}
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\begin{document}$${\gamma}$$\end{document} and Ds(0+)\documentclass[12pt]{minimal}
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\begin{document}$${D_s(0^-)\pi}$$\end{document} and Ds(0-)γ\documentclass[12pt]{minimal}
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\begin{document}$${D_s(0^-)\gamma}$$\end{document} in which leptons are replaced by quarks are also studied. A possibility that the boson near the BB¯\documentclass[12pt]{minimal}
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\begin{document}$${B\bar B}$$\end{document} theshold χb(3P,10.53\documentclass[12pt]{minimal}
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\begin{document}$${\chi_b(3P, 10.53}$$\end{document} GeV) is the Higgs boson partner h0 is discussed. We adopt Dirac lepton neutrinos and Majorana quark neutrinos, and construct a model that satisfy the Z3 symmetry of the lepton sector and the quark sector, by adding two right-handed neutrinos whose left-handed partner cannot be detected by our electro-magnetic detectors.
