2019
DOI: 10.1088/1361-6471/ab4ee8
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Measuring the heavy neutrino oscillations in rare W boson decays at the Large Hadron Collider

Abstract: Majorana neutrinos in the seesaw model can have sizable mixings through which they can be produced at the Large Hadron Collider (LHC) and show a remarkable Lepton Number Violating (LNV) signature. In this article we study the LNV decay of the W boson via two almost degenerate heavy on-shell Majorana neutrinos N j , into three charged leptons and a light neutrino. We consider the scenario where the heavy neutrino masses are within 1 GeV ≤ M N ≤ 10 GeV. We evaluated the possibility to measure a LNV oscillation p… Show more

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Cited by 23 publications
(18 citation statements)
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“…For heavy neutrinos that are produced in W boson decays, the sensitivity is only marginally increased when lowering trigger thresholds, i.e., point iii), because most µ ± from the primary vertex have p T > 25 GeV due to the mass of the W boson. It remains well below what can be achieved in proton collisions at the LHC [76,[78][79][80][81][83][84][85][86][87][88][89][90][91][92].…”
Section: Resultsmentioning
confidence: 78%
“…For heavy neutrinos that are produced in W boson decays, the sensitivity is only marginally increased when lowering trigger thresholds, i.e., point iii), because most µ ± from the primary vertex have p T > 25 GeV due to the mass of the W boson. It remains well below what can be achieved in proton collisions at the LHC [76,[78][79][80][81][83][84][85][86][87][88][89][90][91][92].…”
Section: Resultsmentioning
confidence: 78%
“…In this case the experimentally relevant mixing is U 2 a , the magnitude of which is controlled by the large entries F a . Heavy neutrino oscillations in the detector [58][59][60][61][62][63][64][65][66][67] could provide an indirect way to access the small mass splitting and phenomenologically study this specific case. considered here the upper limit comes from the experimental constraints, while for larger masses there is a theoretical bound U 2 α I < 4π(n − 1)(v/M) 2 from the requirement that the Yukawa couplings remain perturbative [7].…”
Section: The Symmetry Protected Scenariomentioning
confidence: 99%
“…The search for the CP violation has been studied in different scenarios: resonant (overlap) scattering processes [95][96][97], resonant leptonic [98][99][100] and semileptonic rare meson decays [99,101,102], as well as B mesons, W bosons and τ decays that include heavy neutrinos oscillation [60,[103][104][105][106][107][108][109]. The resonant (overlap) effect comes from the interference between two almost degenerate neutrino mass eigenstates with masses of order ∼ GeV.…”
Section: (): V-volmentioning
confidence: 99%