2025/12/15 by Y. Li, Yu-Shuai Li, Li, Yu-Shuai · 1 citation
Physics and Astronomy · #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph)
paper · doi:10.48550/arxiv.2512.13086
In this work, we investigate the two-body nonleptonic decays of double-charmed baryon Ωcc+ within a nonrelativistic quark model, in which the nonfactorizable amplitudes contributed by W-exchange diagrams are evaluated under pole model assumption. To reduce sensitivity of decay amplitudes to arbitrary choice of baryon wave functions, we adopted charmed baryon wave functions obtained by solving the Schrödinger equation with a nonrelativistic quark potential model. Our results show that the branching fractions of CF decays Ωcc+→Ωc0π+ and Ξc(′)+π+, as well as the SCS decays Ωcc+→Ωc0K+, Σcc++K-, Ξc′+η and Λc+K0 can reach up to a few percents. Particularly for the Ωcc+→Ωc0K+ mode, owing to the large factorizable amplitude and constructive pole contributions, the branching fraction is comparable to CF decays. These decay modes can serve as the discovery channels for the double-charmed baryon Ωcc+ in future experiments like LHCb and Belle II.