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- W2091227887 abstract "In supersymmetric quantum chromodynamics (SQCD) with N ``colors'' and M ``flavors'' (N<M), quarks are generated as quasi-Nambu-Goldstone fermions in c${^}_{a}$w${^}_{i}$ and leptons as chiral fermions in ${mathrm{ensuremath{epsilon}}}^{mathrm{abc}}$c${mathrm{^}}_{mathrm{a}}^{mathrm{C}}$c${mathrm{^}}_{mathrm{b}}^{mathrm{C}}$c${mathrm{^}}_{mathrm{c}}^{mathrm{C}}$w${mathrm{^}}_{mathrm{i}}$ (N=4) with antisymmetrized ``colors'' (a=three colors, i=weak isospins). Mass protection symmetry is SU(N-1${)}_{mathrm{L}+mathrm{R}}$ifmmodetimeselsetexttimesfi{}SU(M-N+1${)}_{mathrm{L}}$ifmmodetimeselsetexttimesfi{}SU(M-N+1${)}_{mathrm{R}}$ifmmodetimeselsetexttimesfi{}[Ui(1)'s] supported by complementarity and an effective superpotential. The remaining chiral symmetries are necessarily all broken once supersymmetry is explicitly broken. Masses for quarks and leptons are found to be controlled by the scale ${mathrm{M}}_{mathrm{F}}$=${mathrm{M}}_{mathrm{rSSB}}$(${mathrm{M}}_{mathrm{rSSB}}$/${mathrm{ensuremath{Lambda}}}_{mathrm{rsc}}$${)}^{mathrm{ensuremath{kappa}}}$ with ensuremath{kappa}=(M-N)/[2ensuremath{rho}-(M-N-2)] for 2ensuremath{rho}>M-N-2, where ${M}_{mathrm{SSB}}$ is the supersymmetry-breaking scale and ${ensuremath{Lambda}}_{mathrm{sc}}$ is the scale of SQCD." @default.
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- W2091227887 date "1987-08-01" @default.
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- W2091227887 title "Dynamical model for composite quarks and leptons based on supersymmetric quantum chromodynamics" @default.
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- W2091227887 doi "https://doi.org/10.1103/physrevd.36.932" @default.
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