Search for long-lived particles decaying to e± μ∓ ν

Long-lived particles decaying to $${e ^\pm } {\mu ^\mp } {\nu } $$, with masses between 7 and $$50 \,\text {GeV/}c^2 $$and lifetimes between 2 and $$50 \,\text {ps} $$, are searched for by looking at displaced vertices containing electrons and muons of opposite charges. The search is performed using...

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Hauptverfasser: Aaij, Roel (VerfasserIn) , Archilli, Flavio (VerfasserIn) , Berninghoff, Daniel (VerfasserIn) , Frau, Giulia (VerfasserIn) , Grabowski, Jascha (VerfasserIn) , Han, Xiaoxue (VerfasserIn) , Hu, Jiangqiao (VerfasserIn) , Leverington, Blake (VerfasserIn) , Malygina, Hanna (VerfasserIn) , Stemmle, Simon (VerfasserIn) , Uwer, Ulrich (VerfasserIn) , Witola, Lukas (VerfasserIn)
Körperschaft: LHCb Collaboration (VerfasserIn)
Weitere Verfasser: Schmelling, Michael (BerichterstatterIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 26 March 2021
In: The European physical journal. C, Particles and fields
Year: 2021, Jahrgang: 81, Heft: 3, Pages: 1-16
ISSN:1434-6052
DOI:10.1140/epjc/s10052-021-08994-0
Online-Zugang:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1140/epjc/s10052-021-08994-0
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Verfasserangaben:LHCb Collaboration

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520 |a Long-lived particles decaying to $${e ^\pm } {\mu ^\mp } {\nu } $$, with masses between 7 and $$50 \,\text {GeV/}c^2 $$and lifetimes between 2 and $$50 \,\text {ps} $$, are searched for by looking at displaced vertices containing electrons and muons of opposite charges. The search is performed using $$5.4 \,\text {fb} ^{-1} $$of   |p $$  |p $$collisions collected with the LHCb detector at a centre-of-mass energy of $$\sqrt{s} = 13 \,\text {TeV} $$. Three mechanisms of production of long-lived particles are considered: the direct pair production from quark interactions, the pair production from the decay of a Standard-Model-like Higgs boson with a mass of $$125 \,\text {GeV/}c^2 $$, and the charged current production from an on-shell   |w $$boson with an additional lepton. No evidence of these long-lived states is obtained and upper limits on the production cross-section times branching fraction are set on the different production modes. 
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