Charmed baryon ${\Omega }_c^0\to {\Omega }^{-}{l}^{+}{\nu }_l$ and ${\Omega }_c^0\to {\Omega }_c^{-}{\pi }^{+}({\rho }^{+})$ decays in light cone sum rules

Abstract

The semileptonic ${\Omega }_c^0\to {\Omega }^{-}l\nu$ and non-leptonic ${\Omega }_c^0\to {\Omega }^{-}{\pi }^{+}$, ${\Omega }_c^0\to {\Omega }^{-}{\rho }^{+}$ decays of charmed ${\Omega }_c$ baryon are studied within the light cone sum rules. The form factors responsible for ${\Omega }_c\to \Omega$ transitions are calculated using the distribution amplitudes of ${\Omega }_c$ baryon. With the obtained form factors, the branching ratios of ${\Omega }_c^0\to {\Omega }^{-}{l}^{+}{\nu }_l$, ${\Omega }_c^0\to {\Omega }^{-}{\pi }^{+}$, and ${\Omega }_c^0\to {\Omega }^{-}{\rho }^{+}$ decays are estimated. The results are compared with Belle data as well as the findings of the other approaches.

References in corpus (4)

• Charmed ${\Omega }_c$ weak decays into $\Omega$ in the light-front quark model
• Semileptonic Decays of Heavy Omega Baryons in a Quark Model
• First test of Lepton Flavor Universality in the charmed baryon decays ${\Omega }_c^0\to {\Omega }^{-}{\ell }^{+}{\nu }_{\ell }$ using data of the Belle experiment
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Cited by in corpus (8)

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• Investigating the transition form factors of ${\Lambda }_b\to {\Lambda }_c(2625)$ and ${\Xi }_b\to {\Xi }_c(2815)$ and the corresponding weak decays with support from baryon spectroscopy
• Topological $SU(3{)}_f$ approach for two-body ${\Omega }_c$ weak decays
• Measurement of ${\Omega }_{\mathrm{c}}^0$ baryon production and branching-fraction ratio $\mathrm{BR}({\mathrm{\Omega }}_{\mathrm{c}}^0\to {\mathrm{\Omega }}^{-}{\mathrm{e}}^{+}{\nu }_{\mathrm{e}})/\mathrm{BR}({\mathrm{\Omega }}_{\mathrm{c}}^0\to {\mathrm{\Omega }}^{-}{\pi }^{+})$ in pp collisions at $\sqrt{s}$ = 13 TeV
• Analysis of the strong vertices ${\Lambda }_c{D}^{(\ast )}{N}^{\ast }(1535)$ and ${\Lambda }_b{B}^{(\ast )}{N}^{\ast }(1535)$ in QCD sum rules
• Semileptonic decay of double strangeness heavy flavor baryons
• Analysis of the semileptonic decays ${\Sigma }_b\to {\Sigma }_{c}l{\bar{\nu }}_l$, ${\Xi }_b^{\prime }\to {\Xi }_c^{\prime }l{\bar{\nu }}_l$ and ${\Omega }_b\to {\Omega }_{c}l{\bar{\nu }}_l$ in QCD sum rules