Measurements of branching fractions and asymmetry parameters of Ξ c 0 → Λ K ¯ ∗ 0 $$ {\Xi}_c^0\to \Lambda {\overline{K}}^{\ast 0} $$ , Ξ c 0 → Σ 0 K ¯ ∗ 0 $$ {\Xi}_c^0\to {\Sigma}^0{\overline{K}}^{\ast 0} $$ , and Ξ c 0 → Σ + K ∗ − $$ {\Xi}_c^0\to {\Sigma}^{+}{K}^{\ast -} $$ decays at Belle

Jia S., Tang S. S.,Shen C. P., SOKENDAI (The Graduate University for Advanced Studies), Aihara H., King Abdulaziz University, Asner D. M.,Novosibirsk State University, Aushev T., Ayad R., Babu V.,Bahinipati S., Behera P., Bennett J., Bessner M., Bilka T., Biswal J.,Novosibirsk State University, Bonvicini G.,Bozek A., J. Stefan Institute, Browder T. E., Università di Napoli Federico II, Červenkov D., Chang M.-C., Chekelian V.,Chen A., Cheon B. G., Chilikin K., Cho H. E.,Cho K.,Cho S.-J., Choi S.-K.,Choi Y.,Choudhury S.,Cinabro D.,Cunliffe S.,Das S., Università di Napoli Federico II, Dhamija R., Università di Napoli Federico II,Doležal Z., Dong T. V., P.N. Lebedev Physical Institute of the Russian Academy of Sciences,Novosibirsk State University, Ferber T., Flood K., Fulsom B. G., Garg R., Gaur V.,Novosibirsk State University,Giri A., Goldenzweig P.,Hartbrich O., Hayasaka K., Hayashii H.,Hou W.-S., Hsu C.-L., Iijima T., Inami K., SOKENDAI (The Graduate University for Advanced Studies), Iwasaki M., Iwasaki Y.,Jacobs W. W.,Jin Y., Joo K. K., Karyan G., Kato Y., Kichimi H., Kim C. H.,Kim D. Y., Kim K.-H., Kim S. H.,Kim Y.-K.,Kinoshita K., Kodyš P., Konno T.,Novosibirsk State University, J. Stefan Institute,Novosibirsk State University, J. Stefan Institute,Kroeger R.,Novosibirsk State University,Kuhr T.,Kumara K.,Novosibirsk State University, Kwon Y.-J., Lalwani K., Lange J. S.,Lee S. C., Li J., Li L. K., Li Y. B., Gioi L. Li,Libby J., Lieret K.,High Energy Accelerator Research Organization (KEK), MacQueen C.,Osaka University, Matsuda T., P.N. Lebedev Physical Institute of the Russian Academy of Sciences, McNeil J. T., Università di Napoli Federico II, Metzner F., Miyabayashi K., Miyata H.,National Research University Higher School of Economics, Mohanty G. B., Mussa R., SOKENDAI (The Graduate University for Advanced Studies), Natochii A.,Nayak L., Nayak M., Niiyama M., Nisar N. K., SOKENDAI (The Graduate University for Advanced Studies), Nishimura K., Ogawa K., Ogawa S.,Niigata University, Onuki Y., Oskin P.,Moscow Physical Engineering Institute, P.N. Lebedev Physical Institute of the Russian Academy of Sciences, Pardi S.,Park H.,Park S.-H., Patra S., Max-Planck-Institut für Physik, Pestotnik R., Piilonen L. E., J. Stefan Institute, Popov V., Prencipe E., Prim M. T., Rostomyan A., Rout N., Russo G., Sahoo D., Sandilya S., Sangal A., Savinov V., IKERBASQUE, Basque Foundation for Science, Schwanda C., Seino Y., Senyo K., Sevior M. E., Sharma C., Shiu J.-G., Sokolov A., Solovieva E., Starič M., Stottler Z. S., Sumihama M., Sumiyoshi T.,Meson Science Laboratory, Cluster for Pioneering Research, RIKEN, Tanida K., Tenchini F., Trabelsi K., SOKENDAI (The Graduate University for Advanced Studies),National Research University Higher School of Economics, Unno Y., Uno K., SOKENDAI (The Graduate University for Advanced Studies), Urquijo P.,Novosibirsk State University,Van Tonder R., Varner G., Waheed E., Wang C. H.,Wang M.-Z., Wang P., Watanabe M., Werbycka O., Won E., Yabsley B. D., Yan W., Yang S. B., Ye H., Yelton J., Yin J. H., Yuan C. Z., Yusa Y., Zhang Z. P.,Novosibirsk State University, Zhukova V.

Journal of High Energy Physics(2021)

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摘要
Using a data sample of 980 fb−1 collected with the Belle detector at the KEKB asymmetric-energy e+e− collider, we study the processes of $$ {\Xi}_c^0\to \Lambda {\overline{K}}^{\ast 0} $$ , $$ {\Xi}_c^0\to {\Sigma}^0{\overline{K}}^{\ast 0} $$ , and $$ {\Xi}_c^0\to {\Sigma}^{+}{K}^{\ast -} $$ for the first time. The relative branching ratios to the normalization mode of $$ {\Xi}_c^0\to {\Xi}^{-}{\pi}^{+} $$ are measured to be $$ {\displaystyle \begin{array}{c}\mathcal{B}\left({\Xi}_c^0\to \Lambda {\overline{K}}^{\ast 0}\right)/\mathcal{B}\left({\Xi}_c^0\to {\Xi}^{-}{\pi}^{+}\right)=0.18\pm 0.02\left(\mathrm{stat}.\right)\pm 0.01\left(\mathrm{syst}.\right),\\ {}\mathcal{B}\left({\Xi}_c^0\to {\Sigma}^0{\overline{K}}^{\ast 0}\right)/\mathcal{B}\left({\Xi}_c^0\to {\Xi}^{-}{\pi}^{+}\right)=0.69\pm 0.03\left(\mathrm{stat}.\right)\pm 0.03\left(\mathrm{syst}.\right),\\ {}\mathcal{B}\left({\Xi}_c^0\to {\Sigma}^{+}{K}^{\ast -}\right)/\mathcal{B}\left({\Xi}_c^0\to {\Xi}^{-}{\pi}^{+}\right)=0.34\pm 0.06\left(\mathrm{stat}.\right)\pm 0.02\left(\mathrm{syst}.\right),\end{array}} $$ where the uncertainties are statistical and systematic, respectively. We obtain $$ {\displaystyle \begin{array}{c}\mathcal{B}\left({\Xi}_c^0\to \Lambda {\overline{K}}^{\ast 0}\right)=\left(3.3\pm 0.3\left(\mathrm{stat}.\right)\pm 0.2\left(\mathrm{syst}.\right)\pm 1.0\left(\mathrm{ref}.\right)\right)\times {10}^{-3},\\ {}\mathcal{B}\left({\Xi}_c^0\to {\Sigma}^0{\overline{K}}^{\ast 0}\right)=\left(12.4\pm 0.5\left(\mathrm{stat}.\right)\pm 0.5\left(\mathrm{syst}.\right)\pm 3.6\left(\mathrm{ref}.\right)\right)\times {10}^{-3},\\ {}\mathcal{B}\left({\Xi}_c^0\to {\Sigma}^{+}{K}^{\ast 0}\right)=\left(6.1\pm 1.0\left(\mathrm{stat}.\right)\pm 0.4\left(\mathrm{syst}.\right)\pm 1.8\left(\mathrm{ref}.\right)\right)\times {10}^{-3},\end{array}} $$ where the uncertainties are statistical, systematic, and from $$ \mathcal{B}\left({\Xi}_c^0\to {\Xi}^{-}{\pi}^{+}\right) $$ , respectively. The asymmetry parameters $$ \alpha \left({\Xi}_c^0\to \Lambda {\overline{K}}^{\ast 0}\right) $$ and $$ \alpha \left({\Xi}_c^0\to {\Sigma}^{+}{K}^{\ast -}\right) $$ are 0.15 ± 0.22(stat.) ± 0.04(syst.) and −0.52 ± 0.30(stat.) ± 0.02(syst.), respectively, where the uncertainties are statistical followed by systematic.
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关键词
Branching fraction, e +-e Experiments, Charm physics
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