Observation of $\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}$ and $\Xi(1530)^{-}\bar\Xi^{+}$
dc.contributor.author | Ablikim, M. | |
dc.contributor.author | Mitchell, R. E., et al | |
dc.date.accessioned | 2025-02-20T16:12:07Z | |
dc.date.available | 2025-02-20T16:12:07Z | |
dc.date.issued | 2019-09-26 | |
dc.description.abstract | Using $448.1 × 10^6$ $\psi(3686)$ events collected with the BESIII detector at BEPCII, we employ a single-baryon tagging technique to make the first observation of $\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}$ and $\Xi(1530)^{-}\bar\Xi^{+}$ decays with a statistical significance of more than 10$\sigma$ and 5.0$\sigma$, respectively. The branching fractions are measured to be $\cal{B}$$[\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}]$ $=$ $(11.45 ± 0.40 ± 0.59) × 10^{−5}$ and $\cal{B}$$[\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi^{+}]$ $=$ $(0.70 ± 0.11 ± 0.04) × 10^{−5}$. The angular distribution parameter for $\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}$ is determined to be $\alpha$ = 0.40 ± 0.24 ± 0.06, which agrees with the theoretical predictions within 1$\sigma$. The first uncertainties are statistical, and the second systematic. | |
dc.identifier.citation | Ablikim, M., and Mitchell, R. E., et al. "Observation of $\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}$ and $\Xi(1530)^{-}\bar\Xi^{+}$." Physical Review D, vol. D100, no. 5, 2019-09-26, https://doi.org/10.1103/PhysRevD.100.051101. | |
dc.identifier.issn | 2470-0010 | |
dc.identifier.other | BRITE 6202 | |
dc.identifier.uri | https://hdl.handle.net/2022/31836 | |
dc.language.iso | en | |
dc.relation.isversionof | https://doi.org/10.1103/PhysRevD.100.051101 | |
dc.relation.isversionof | https://journals.aps.org/prd/abstract/10.1103/PhysRevD.100.051101 | |
dc.relation.journal | Physical Review D | |
dc.title | Observation of $\psi(3686)\rightarrow\Xi(1530)^{-}\bar\Xi(1530)^{+}$ and $\Xi(1530)^{-}\bar\Xi^{+}$ |
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