Evidence for the singly Cabibbo-suppressed decay $$ {\Omega}_c^0\to {\Xi}^{-}{\pi}^{+} $$ and search for $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ and Ω−K+ decays at Belle

Author:

,Han X.,Jia S.,Yuan L.,Shen C. P.,Adachi I.,Ahn J. K.,Aihara H.,Asner D. M.,Aushev T.,Ayad R.,Babu V.,Bahinipati S.,Banerjee Sw.,Behera P.,Belous K.,Bennett J.,Bessner M.,Bhardwaj V.,Bilka T.,Biswas D.,Bodrov D.,Borah J.,Bračko M.,Branchini P.,Browder T. E.,Budano A.,Campajola M.,Červenkov D.,Chang M.-C.,Chang P.,Chen A.,Cheon B. G.,Chilikin K.,Cho H. E.,Cho K.,Choi S.-K.,Choi Y.,Choudhury S.,Cinabro D.,De Nardo G.,De Pietro G.,Dhamija R.,Di Capua F.,Doležal Z.,Dong T. V.,Epifanov D.,Ferber T.,Ferlewicz D.,Fulsom B. G.,Gaur V.,Giri A.,Goldenzweig P.,Graziani E.,Gu T.,Hadjivasiliou C.,Hara T.,Hayasaka K.,Hayashii H.,Hou W.-S.,Hsu C.-L.,Iijima T.,Inami K.,Ipsita N.,Ishikawa A.,Itoh R.,Iwasaki M.,Jacobs W. W.,Jang E.-J.,Ji Q. P.,Jin Y.,Kaliyar A. B.,Kiesling C.,Kim C. H.,Kim D. Y.,Kim Y.-K.,Kinoshita K.,Kodyš P.,Konno T.,Korobov A.,Korpar S.,Kovalenko E.,Križan P.,Krokovny P.,Kuhr T.,Kumar M.,Kumar R.,Kumara K.,Kwon Y.-J.,Lam T.,Laurenza M.,Lee S. C.,Li C. H.,Li J.,Li L. K.,Li S. X.,Li Y.,Li Y. B.,Gioi L. Li,Libby J.,Lieret K.,Masuda M.,Maurya S. K.,Merola M.,Miyabayashi K.,Mizuk R.,Mohanty G. B.,Mussa R.,Nakamura I.,Nakao M.,Nakazawa H.,Natkaniec Z.,Natochii A.,Nisar N. K.,Nishida S.,Ogawa S.,Ono H.,Onuki Y.,Pakhlova G.,Park H.,Park J.,Patra S.,Paul S.,Pedlar T. K.,Pestotnik R.,Piilonen L. E.,Prencipe E.,Prim M. T.,Rout N.,Russo G.,Sandilya S.,Santelj L.,Savinov V.,Schnell G.,Schueler J.,Schwanda C.,Seino Y.,Senyo K.,Sevior M. E.,Shan W.,Shapkin M.,Sharma C.,Shiu J.-G.,Shwartz B.,Solovieva E.,Starič M.,Sumihama M.,Sumiyoshi T.,Takizawa M.,Tanida K.,Tenchini F.,Trabelsi K.,Uchida M.,Uglov T.,Unno Y.,Uno K.,Uno S.,Urquijo P.,Vahsen S. E.,van Tonder R.,Varner G.,Vinokurova A.,Wang X. L.,Won E.,Yabsley B. D.,Yan W.,Yang S. B.,Yelton J.,Yin J. H.,Yuan C. Z.,Zhang Z. P.,Zhilich V.,Zhukova V.

Abstract

Abstract Using a data sample of 980 fb1 collected with the Belle detector at the KEKB asymmetric-energy e+e collider, we study for the first time the singly Cabibbo-suppressed decays $$ {\Omega}_c^0\to {\Xi}^{-}{\pi}^{+} $$ Ω c 0 Ξ π + and ΩK+ and the doubly Cabibbo-suppressed decay $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ Ω c 0 Ξ K + . Evidence for an $$ {\Omega}_c^0 $$ Ω c 0 signal in the $$ {\Omega}_c^0 $$ Ω c 0 Ξπ+ mode is reported with a significance of 4.5σ including systematic uncertainties. The ratio of branching fractions to the normalization mode $$ {\Omega}_c^0 $$ Ω c 0 Ωπ+ is measured to be$$ \mathcal{B}\left({\Omega}_c^0\to {\Xi}^{-}{\pi}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)=0.253\pm 0.052\left(\textrm{stat}.\right)\pm 0.030\left(\textrm{syst}.\right). $$ B Ω c 0 Ξ π + / B Ω c 0 Ω π + = 0.253 ± 0.052 stat . ± 0.030 syst . . No significant signals of $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ Ω c 0 Ξ K + and ΩK+ modes are found. The upper limits at 90% confidence level on ratios of branching fractions are determined to be$$ \mathcal{B}\left({\Omega}_c^0\to {\Xi}^{-}{K}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)<0.070 $$ B Ω c 0 Ξ K + / B Ω c 0 Ω π + < 0.070 and$$ \mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{K}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)<0.29. $$ B Ω c 0 Ω K + / B Ω c 0 Ω π + < 0.29 .

Publisher

Springer Science and Business Media LLC

Subject

Nuclear and High Energy Physics

Reference31 articles.

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