Hidden strangeness in meson weak decays to baryon pair
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2024
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| _version_ | 1866916505173622784 |
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| author | Geng, Chao-Qiang Jin, Xiang-Nan Liu, Chia-Wei Yu, Xiao |
| author_facet | Geng, Chao-Qiang Jin, Xiang-Nan Liu, Chia-Wei Yu, Xiao |
| contents | Our study focuses on the weak decay of $ D_s^+ \to p \overline{n} $, which is the only possible two-body baryonic decay in the $ D $ meson system. An analysis using perturbative quantum chromodynamics (pQCD) is challenging in this decay due to the small amount of energy released. In particular, naive factorization, suppressed by the light quark masses, results in a minor contribution to this channel. In the framework of final state interactions, the hidden strangeness in the intermediate state naturally avoids this chiral suppression from light quark masses. The branching fraction is predicted to be $ {\cal B}(D_s^+ \to p\overline{n}) = (1.43 \pm 0.10) \times 10^{-3} $, in agreement with the experimental value of $ (1.22 \pm 0.11) \times 10^{-3} $. We also analyze the decays of $ B $ mesons into two charmed baryons involving annihilation-type topological diagrams. In these decays, we conduct a joint analysis of naive factorization and final state interactions. Using the experimental upper bound of $ {\cal B}(B_s^0 \to Λ_c^+ \overlineΛ_c^-) < 8 \times 10^{-5} $, we set a constraint on the coupling constant $ g_{D^+ Λ_c^+ n} < 7.5 $. Final state interactions lead to a prediction of the decay parameter $ γ(B_s^0 \to Λ_c^+ \overlineΛ_c^-) > 0.8 $, whereas pQCD predicts it to be negative. We propose future measurements of $ B^0 \to Ξ_c^+ \overlineΞ_c^- $, predicting a significant $ SU(3)_F $ breaking effect with $ \frac{{\cal B}(B^0 \to Ξ_c^+ \overlineΞ_c^-)}{{\cal B}(B_s^0 \to Λ_c^+ \overlineΛ_c^-)} = 1.4\% $, contrary to the naive estimate of $ 5.3\% $. We strongly recommend future measurements. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2409_11374 |
| institution | arXiv |
| publishDate | 2024 |
| record_format | arxiv |
| spellingShingle | Hidden strangeness in meson weak decays to baryon pair Geng, Chao-Qiang Jin, Xiang-Nan Liu, Chia-Wei Yu, Xiao High Energy Physics - Phenomenology High Energy Physics - Experiment Our study focuses on the weak decay of $ D_s^+ \to p \overline{n} $, which is the only possible two-body baryonic decay in the $ D $ meson system. An analysis using perturbative quantum chromodynamics (pQCD) is challenging in this decay due to the small amount of energy released. In particular, naive factorization, suppressed by the light quark masses, results in a minor contribution to this channel. In the framework of final state interactions, the hidden strangeness in the intermediate state naturally avoids this chiral suppression from light quark masses. The branching fraction is predicted to be $ {\cal B}(D_s^+ \to p\overline{n}) = (1.43 \pm 0.10) \times 10^{-3} $, in agreement with the experimental value of $ (1.22 \pm 0.11) \times 10^{-3} $. We also analyze the decays of $ B $ mesons into two charmed baryons involving annihilation-type topological diagrams. In these decays, we conduct a joint analysis of naive factorization and final state interactions. Using the experimental upper bound of $ {\cal B}(B_s^0 \to Λ_c^+ \overlineΛ_c^-) < 8 \times 10^{-5} $, we set a constraint on the coupling constant $ g_{D^+ Λ_c^+ n} < 7.5 $. Final state interactions lead to a prediction of the decay parameter $ γ(B_s^0 \to Λ_c^+ \overlineΛ_c^-) > 0.8 $, whereas pQCD predicts it to be negative. We propose future measurements of $ B^0 \to Ξ_c^+ \overlineΞ_c^- $, predicting a significant $ SU(3)_F $ breaking effect with $ \frac{{\cal B}(B^0 \to Ξ_c^+ \overlineΞ_c^-)}{{\cal B}(B_s^0 \to Λ_c^+ \overlineΛ_c^-)} = 1.4\% $, contrary to the naive estimate of $ 5.3\% $. We strongly recommend future measurements. |
| title | Hidden strangeness in meson weak decays to baryon pair |
| topic | High Energy Physics - Phenomenology High Energy Physics - Experiment |
| url | https://arxiv.org/abs/2409.11374 |