Observation of the decay Λ0b → χc1pπ−

Roel Aaij,C. Abellán Beteta,Thomas Ackernley,Bernardo Adeva,Marco Adinolfi,Hossein Afsharnia,C. A. Aidala,Salvatore Aiola,Ziad Ajaltouni,Simon Akar,Johannes Albrecht,Federico Alessio,Michael Alexander,A. Alfonso Albero, Zakariya Aliouche, G. Alkhazov,P. Alvarez Cartelle,Sandra Amato,Yasmine Amhis,Liupan An,Lucio Anderlini, Aleksei Andreianov, M. Andreotti, F. Archilli,A. Artamonov,Marina Artuso, Kenenbek Arzymatov,Elie Aslanides,Michele Atzeni,Benjamin Audurier,Sebastian Bachmann,Marie Bachmayer,J. J. Back,P. Baladron Rodriguez,V. Balagura,W. Baldini,J. Baptista Leite,R. J. Barlow,Sergey Barsuk,William Barter,Matteo Bartolini,Fedor Baryshnikov, Jan-Marc Basels,Giovanni Bassi, Baasansuren Batsukh,Alexander Battig, A. Bay,Michael Becker,Franco Bedeschi,Ignacio Bediaga,Andrew Beiter,Vladislav Belavin,Samuel Belin,Violaine Bellee, K. Belous,Ilia Belov,Ivan Belyaev, G. Bencivenni, E. Ben-Haim,Alexander Berezhnoy,Roland Bernet,Daniel Berninghoff, Harris Conan Bernstein,Claudia Bertella,A. Bertolin,Christopher Betancourt,Federico Betti,Ia. Bezshyiko,Srishti Bhasin,Jihyun Bhom, L. Bian,Martin Stefan Bieker,Simone Bifani, P. Billoir, Matthew Birch, Fionn Caitlin Ros Bishop,A. Bitadze,Andrea Bizzeti,Mikkel Bjørn,Michele Piero Blago,Thomas Blake,F. Blanc,S. Blusk, Dana Bobulska, Julian Alexander Boelhauve,O. Boente Garcia, T. Boettcher,Alexey Boldyrev, A. Bondar,Nikolay Bondar,Silvia Borghi,Maxim Borisyak,Martino Borsato,Jozef Tomasz Borsuk, Sonia Amina Bouchiba,T. J. V. Bowcock,Alexandre Boyer, C. Bozzi, M. J. Bradley

Journal of High Energy Physics(2021)

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摘要
The Cabibbo-suppressed decay $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc1pπ− 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 $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc2pπ− decay is also found. Using the $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc1pK− 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 χc1,2 → J/ψγ decays.
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