Observation of the Z → ψ ℓ + ℓ - decay in pp collisions at v s = 13 TeV

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, colle...

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Bibliographic Details
Main Author: CMS Collaboration (Author)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2020-04-24T17:44:51Z.
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Online Access:Get fulltext
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100 1 0 |a CMS Collaboration  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
245 0 0 |a Observation of the Z → ψ ℓ + ℓ - decay in pp collisions at v s = 13 TeV 
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520 |a 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 
546 |a en_US 
655 7 |a Article 
773 |t 10.1103/PhysRevLett.121.141801 
773 |t Physical review letters