Observation of the decay $\Lambda_b^0\rightarrow\chi_{c1}p\pi^-$

Diego Torres Machado,Matthew John Bradley,Gregory Ciezarek, Maciej Wojciech Dudek, P. Collins,Steffen Georg Weber,Wenbin Qian, Halime Sazak,Simone Meloni,Tomasz Szumlak, Jennifer Clare Smallwood,Serena Maccolini,Lakshan Ram Madhan Mohan,Marcel Merk,Paula Garcia Moreno,Alexander Bitadze,Konstantin Gizdov, Marie-Noelle Minard,Daniel Berninghoff,Pavel Krokovny,Gianfranco Morello,Andrea Merli, Tamaki Holly Mcgrath,Thi Dung Nguyen, Carmen Giugliano,Roel Aaij, Ryan Newcombe, Guillaume Pietrzyk, Paul Nathaniel Swallow,Leonid Kravchuk,Tatiana Ovsiannikova,Mikkel Bjørn,Shuangli Yang,Menglin Xu,Yutong Li, Ivan Polyakov,Veronika Chobanova,Thomas Kirn, Kara Renee Mattioli,Matteo Palutan,Luke George Scantlebury Smead,Vladimir Romanovskiy, Adam Dendek,Mauro Piccini,Sebastian Bachmann,Marie Bachmayer,Zhenzi Wang,Carina Trippl,Kazuyoshi Carvalho Akiba,Timothy Evans,Giovanni Punzi,Da Yu Tou,Neville Harnew,Stephan Escher, Fionn Caitlin Ros Bishop,Marcin Chrzaszcz,Alexandre Boyer,Sune Jakobsen,Guido Haefeli,Sheldon Stone,Marek Idzik,Jennifer Brigitta Zonneveld,Guanghua Gong,Florin Maciuc, Marcel Materok,Davide Pinci,Miriam Lucio Martinez, Eduard Ursov,Hangyi Wu,Yangheng Zheng,Daniel Patrick O'Hanlon, Daria Strekalina,Jeremy Dalseno,Roland Waldi,Sergei Popov,Nikolay Nikitin, Sara Elizabeth Mitchell, Vladimir Chulikov, Louis Lenard Gerken,Michele Atzeni,Stephen M. Stahl,Sebastian Neubert,Artur Ishteev,Christopher Jones,Christoph Langenbruch, Robbert Erik Geertsema,Mikhail Zavertyaev,Eluned Smith,Tai-Hua Lin,Margarete Schellenberg,Anna Danilina, Jascha Peter Grabowski, Jan-Marc Basels,Matthew Needham,Burkhard Schmidt,Domenico Galli,Christoph Hasse,Thomas Ackernley,Tabitha Halewood-leagas, Cheryl Pappenheimer

Journal of High Energy Physics(2021)

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摘要
The Cabibbo-suppressed decay $ {\Lambda}_{\mathrm{b}}^0 $→ χ$_{c1}$pπ$^{−}$ is observed for the first time using data from proton-proton collisions corresponding to an integrated luminosity of 6 fb$^{−1}$, collected with the LHCb detector at a centre-of-mass energy of 13 TeV. Evidence for the $ {\Lambda}_{\mathrm{b}}^0 $→ χ$_{c2}$pπ$^{−}$ decay is also found. Using the $ {\Lambda}_{\mathrm{b}}^0 $→ χ$_{c1}$pK$^{−}$ decay as normalisation channel, the ratios of branching fractions are measured to be$ {\displaystyle \begin{array}{c}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=\left(6.59\pm 1.01\pm 0.22\right)\times {10}^{-2}, {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}=0.95\pm 0.30\pm 0.04\pm 0.04, {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\mathrm{K}}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=1.06\pm 0.05\pm 0.04\pm 0.04,\end{array}} $where the first uncertainty is statistical, the second is systematic and the third is due to the uncertainties in the branching fractions of χ$_{c1,2}$→ J/ψγ decays.[graphic not available: see fulltext]
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