Repository logo
Log in(current)
Repository logoMIT Open ScholarshipDSpace@MIT
  1. Home
  2. MIT Open Access Articles
  3. MIT Open Access Articles
  4. Observation of the decay Λ b 0 $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc1pπ−

Observation of the decay Λ b 0 $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc1pπ−

Thumbnail Image
Download
Name

13130_2021_Article_15658.pdf

Size

494.87 KB

Format

Adobe PDF

Checksum (MD5)

e809b540bea196400868979d46074f4c

Download all files submitted through automated deposit
art_5183501315126369843.zip (390.18 KB)
Author(s)
Aaij, R.
•
Abellán Beteta, C.
•
Ackernley, T.
•
Adeva, B.
•
Adinolfi, M.
•
Afsharnia, H.
•
Aidala, C. A
•
Aiola, S.
•
Ajaltouni, Z.
•
Akar, S.
more
Date Issued
May 12, 2021
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2021 May 12;2021(5):95
Version
Final published version
Abstract
Abstract The Cabibbo-suppressed decay Λ b 0 $$ {\Lambda}_{\mathrm{b}}^0 $$ → 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 Λ b 0 $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc2pπ− decay is also found. Using the Λ b 0 $$ {\Lambda}_{\mathrm{b}}^0 $$ → χc1pK− decay as normalisation channel, the ratios of branching fractions are measured to be B Λ b 0 → χ c 1 pπ − B Λ b 0 → χ c 1 pK − = 6.59 ± 1.01 ± 0.22 × 10 − 2 , B Λ b 0 → χ c 2 pπ − B Λ b 0 → χ c 1 pπ − = 0.95 ± 0.30 ± 0.04 ± 0.04 , B Λ b 0 → χ c 2 pK − B Λ b 0 → χ c 1 pK − = 1.06 ± 0.05 ± 0.04 ± 0.04 , $$ {\displaystyle \begin{array}{c}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=\left(6.59\pm 1.01\pm 0.22\right)\times {10}^{-2},\\ {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\uppi}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\uppi}^{-}\right)}=0.95\pm 0.30\pm 0.04\pm 0.04,\\ {}\frac{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}2}{\mathrm{p}\mathrm{K}}^{-}\right)}{\mathcal{B}\left({\Lambda}_{\mathrm{b}}^0\to {\upchi}_{\mathrm{c}1}{\mathrm{p}\mathrm{K}}^{-}\right)}=1.06\pm 0.05\pm 0.04\pm 0.04,\end{array}} $$ 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.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution
https://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
https://hdl.handle.net/1721.1/136799
DOI of Published Version
https://doi.org/10.1007/JHEP05(2021)095
Repository logo
PrivacyPermissionsAccessibilityContact us
Repository logo
Notify us about copyright concerns.