Two-body charmed baryon decays involving vector meson with $SU(3)$ flavor symmetry
Abstract: We study the two-body anti-triplet charmed baryon decays of ${\bf B}c\to {\bf B}_n V$, with ${\bf B}_c=(\Xi_c{0},-\Xi_c{+},\Lambda_c+)$ and ${\bf B}_n(V)$ the baryon (vector meson) states. Based on the $SU(3)$ flavor symmetry, we predict that ${\cal B}(\Lambda{+}{c}\to \Sigma{+}\rho{0},\Lambda0 \rho+)=(0.61\pm 0.46,0.74\pm 0.34)\%$, in agreement with the experimental upper bounds of $(1.7,6)\%$, respectively. We also find ${\cal B}(\Lambda+_c \to \Xi0 K{*+},\Sigma0 K{*+},\Lambda0 K{*+}) =(8.7 \pm 2.7,1.2\pm 0.3,2.0\pm 0.5)\times 10{-3}$ to be compatible with the pseudoscalar counterparts. For the doubly Cabibbo-suppressed decay $\Xi+_c \to p\phi$, measured for the first time, we predict its branching ratio to be $(1.5\pm 0.7)\times 10{-4}$, together with ${\cal B}(\Xi+_c \to p \bar K{*0},\Sigma+ \phi) =(7.8 \pm 2.2,1.9\pm0.9)\times 10{-3}$. The ${\bf B}_c\to{\bf B}_n V$ decays with ${\cal B}\simeq {\cal O}(10{-4}-10{-3})$ are accessible to the BESIII, BELLEII and LHCb experiments.
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