2019
DOI: 10.1140/epjc/s10052-019-7422-z
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Lepton flavor violation and collider searches in a type I + II seesaw model

Abstract: Neutrino are massless in the Standard Model. The most popular mechanism to generate neutrino masses are the type I and type II seesaw, where right-handed neutrinos and a scalar triplet are augmented to the Standard Model, respectively. In this work, we discuss a model where a type I + II seesaw mechanism naturally arises via spontaneous symmetry breaking of an enlarged gauge group. Lepton flavor violation is a common feature in such setup and for this reason, we compute the model contribution to the µ → eγ and… Show more

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Cited by 19 publications
(7 citation statements)
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References 113 publications
(120 reference statements)
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“…The consideration of different mass hiearchies will not bring much impact to our paper which focuses on the proposition of a new 2HDM model. Anyways, strictly speaking, one should keep in mind that different mass hierarchies are subject to different collider bounds as pointed out [93]. Anyway, if we find ourselves in a situation where both doubly charged scalar and Z fields are observed, our model stands as a potential well motivated environment for them.…”
Section: Lhc -Doubly Charged Scalarmentioning
confidence: 92%
“…The consideration of different mass hiearchies will not bring much impact to our paper which focuses on the proposition of a new 2HDM model. Anyways, strictly speaking, one should keep in mind that different mass hierarchies are subject to different collider bounds as pointed out [93]. Anyway, if we find ourselves in a situation where both doubly charged scalar and Z fields are observed, our model stands as a potential well motivated environment for them.…”
Section: Lhc -Doubly Charged Scalarmentioning
confidence: 92%
“…[88][89][90] for classic phenomenological studies and Refs. [91][92][93][94][95][96] for projections of H ±± at future hadron colliders). At the low-energy high-precision frontier, the coupling f αβ is also constrained by the LFV decays α → β γ, α → β γ δ , the electron and muon g − 2, muonium oscillation, and the LEP e + e − → + − data (see e.g., Ref.…”
Section: Doubly Charged Scalar H ±±mentioning
confidence: 99%
“…This inequality needs to be checked after each fit to make sure that the found parameter values are acceptable. Furthermore, there are experimental bounds on the parameters related to the SU(2) L triplet: v L 1 GeV and M ∆ 1 TeV [58,59]. Finally, the vev v R should be set to M GUT .…”
Section: Jhep09(2021)111mentioning
confidence: 99%