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  4. Measurement of the ratio of the production cross sections times branching fractions of B [superscript ±][subscript c] → [J over ψπ [superscript ±]] and B[superscript ±] → [J over ψK [superscript ±]] and ℬ(B [superscript ±][subscript c] → [J over Ψ π [superscript ±] π [superscript ±] π [superscript ∓] [over ℬ(B [superscript ±][subscript c] → J [over Ψ π [superscript ±]]) in pp collisions at √s = 7 TeV

Measurement of the ratio of the production cross sections times branching fractions of B [superscript ±][subscript c] → [J over ψπ [superscript ±]] and B[superscript ±] → [J over ψK [superscript ±]] and ℬ(B [superscript ±][subscript c] → [J over Ψ π [superscript ±] π [superscript ±] π [superscript ∓] [over ℬ(B [superscript ±][subscript c] → J [over Ψ π [superscript ±]]) in pp collisions at √s = 7 TeV

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Author(s)
Apyan, Aram
•
Busza, Wit
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Cali, Ivan Amos
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Chan, M.
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Di Matteo, Leonardo
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Gomez-Ceballos, Guillelmo
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Goncharov, Maxim
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Gulhan, Doga Can
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Klute, Markus
•
Lai, Yue Shi
more
Date Issued
January 2015
Journal
Journal of High Energy Physics
Publisher
Springer-Verlag
Citation
The CMS collaboration et al. “Measurement of the Ratio of the Production Cross Sections Times Branching Fractions of B [superscript ±][subscript c] → [J over ψπ [superscript ±]] and B[superscript ±] → [J over ψK [superscript ±]] and ℬ(B [superscript ±][subscript c] → [J over Ψ π [superscript ±] π [superscript ±] π [superscript ∓] [over ℬ(B [superscript ±][subscript c] → J [over Ψ π [superscript ±]]) in Pp Collisions at √s = 7 TeV.” Journal of High Energy Physics 2015.1 (2015): 1-13.
Version
Final published version
Abstract
The ratio of the production cross sections times branching fractions (σ(B[superscript ± [subscript c])B(B[superscript ±] [subscript c]→J[over ψπ [superscript ±]])) [over (σ(B [superscript ±])B(B[superscript ±]→J/ψK[superscript ±]))] is studied in proton-proton collisions at a center-of-mass energy of 7 TeV with the CMS detector at the LHC. The kinematic region investigated requires B [subscript c] [superscript ±] and B[superscript ±] mesons with transverse momentum p [subscript T] > 15 GeV and rapidity |y| < 1.6. The data sample corresponds to an integrated luminosity of 5.1 fb [superscript −1]. The ratio is determined to be [0.48±0.05(stat)±0.03(syst)±0.05 (τB[subscript c])]% . The B [subscript c] [superscript ±]  → J [over ψπ [superscript ±] π [superscript ±] π [superscript ∓]] decay is also observed in the same data sample. Using a model-independent method developed to measure the efficiency given the presence of resonant behaviour in the three-pion system, the ratio of the branching fractions B(B[superscript ±][subscript c]→J [over ψπ [superscript ±] π [superscript ±] π [superscript ∓]]) [over B(B[superscript ±] [subscript c] →J [over ψπ[superscript ±]])] is measured to be 2.55±0.80(stat)±0.33(syst)[superscript +0.04][subscript −0.01](τB[subscript c]) , consistent with the previous LHCb result.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Massachusetts Institute of Technology. School of Science
Terms of Use
Creative Commons Attribution
http://creativecommons.org/licenses/by/4.0/
Persistent DSpace Link
http://hdl.handle.net/1721.1/94584
DOI of Published Version
https://doi.org/10.1007/JHEP01(2015)063
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