Measurements of branching fractions and asymmetry parameters 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 -} $ decays at Belle

S. Jia, S. S. Tang,C. P. Shen,Iki Adachi, H. Aihara,S. Al Said, D. M. Asner, V.M. Aulchenko,Tagir Aushev, R. Ayad, V. Babu,Seema Bahinipati,Prafulla Kumar Behera, J. Bennett, M. Bessner,T. Bilka, J. Biswal,A. Bobrov, G. Bonvicini, A. Bozek, M. Bračko,T. E. Browder,M. Campajola, D. Červenkov,M. C. Chang, V. Chekelian,A. Chen,B. G. Cheon, K. Chilikin, H. E. Cho,K. Cho,S.-J. Cho,S. K. Choi,Y. Choi,Somnath Choudhury,D. Cinabro,S. Cunliffe,S. Das,G. De Nardo, R. Dhamija,F. Di Capua, Z. Doležal, T. V. Dong,Semen Eidelman,D. Epifanov, T. Ferber, K. Flood,B. G. Fulsom,Rocky Bala Garg, V. Gaur, N. Gabyshev, A. Garmash, A. K. Giri, P. Goldenzweig,O. Hartbrich, K. Hayasaka, H. Hayashii,W. S. Hou,C.-L. Hsu,T. Iijima, K. Inami,A. Ishikawa, R. Itoh,M. Iwasaki, Y. Iwasaki,W. W. Jacobs, Y. Jin,K. K. Joo, G. Karyan, Y. Kato,H. Kichimi,C. H. Kim,D. Y. Kim,K.-H. Kim,Seok Kim,Yongsun Kim,K. Kinoshita,Peter Kodys,Tomoyuki Konno,A. Korobov,Samo Korpar,E. Kovalenko, P. Križan,R. Kroeger, P. Krokovny, T. Kuhr,K. Kumara,A. Kuzmin,Y. J. Kwon, K. Lalwani,J. S. Lange,Shih-Chang Lee,J. Li,L. K. Li, Y. B. Li,L. Li Gioi, J. Libby, K. Lieret, D. Liventsev, C. MacQueen

Journal of High Energy Physics(2021)

引用 2|浏览8
暂无评分
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.
更多
查看译文
关键词
Branching fraction,e +-e Experiments,Charm physics
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要