Observation of the Z → ψ ℓ + ℓ - decay in pp collisions at v s = 13 TeV
Name
PhysRevLett.121.141801.pdf
Size
443.7 KB
Format
Adobe PDF
Checksum (MD5)
839bf938a59f5c93ef2af41e4c13e313
Author(s)
CMS Collaboration
Date Issued
October 2018
Journal
Physical review letters
Publisher
American Physical Society
Citation
CMS Collaboration (Sirunyan, A.M., et al.), "Observation of the Z → ψ ℓ + ℓ - decay in pp collisions at v s = 13 TeV." Physical review letters 121 (2018): letter 121 doi 10.1103/PhysRevLett.121.141801 ©2018 Author(s)
Version
Final published version
Abstract
This Letter presents the observation of the rare Z boson decay Z→ ψ ℓ + ℓ − . Here, ψ represents contributions from direct J/ψ and ψ ( 2 S ) → J / ψ X , ℓ + ℓ − is a pair of electrons or muons, and the J/ψ meson is detected via its decay to μ + μ − . The sample of proton-proton collision data, collected by the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponds to an integrated luminosity of 35.9 fb − 1 . The signal is observed with a significance in excess of 5 standard deviations. After subtraction of the ψ ( 2 S ) → J / ψ X contribution, the ratio of the branching fraction of the exclusive decay Z→ J / ψ ℓ + ℓ − to the decay Z→ μ + μ − μ + μ − within a fiducial phase space is measured to be B(Z→ J / ψ ℓ + ℓ − ) / B ( Z → μ + μ − μ + μ − ) = 0.67 ± 0.18 ( stat ) ± 0.05 ( syst ). ©2018
MIT Department
Massachusetts Institute of Technology. Department of Physics
Terms of Use
Creative Commons Attribution 3.0 unported license
Persistent DSpace Link
DOI of Published Version
https://doi.org/10.1103/PhysRevLett.121.141801