Derives U-spin sum rules for bottom baryon two-body decays via effective Hamiltonian operators, yielding branching fraction predictions and CP asymmetry relations beyond the symmetry limit.
INTRODUCTION Nonleptonic decays of bottom baryons provide laboratories for studying strong and weak interactions in heavy- to-light baryonic transitions
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$U$-spin sum rules for two-body decays of bottom baryons
Derives U-spin sum rules for bottom baryon two-body decays via effective Hamiltonian operators, yielding branching fraction predictions and CP asymmetry relations beyond the symmetry limit.