2018
DOI: 10.1103/physrevd.98.015024
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Probing the type-II seesaw mechanism through the production of Higgs bosons at a lepton collider

Abstract: We investigate the production and decays of doubly-charged Higgs bosons for the Type-II seesaw mechanism at an e þ e − collider with two center of mass energies, ffiffi ffi s p ¼ 380 GeV and 3 TeV, and analyze the fully hadronic final states in detail. Lower mass ranges can be probed during the 380 GeV run of the collider, while high mass ranges, which are beyond the 13 TeV Large Hadron Collider discovery reach, can be probed with ffiffi ffi s p ¼ 3 TeV. For such a heavy Higgs boson, the final decay products a… Show more

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Cited by 29 publications
(20 citation statements)
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“…This difference in the lower mass bound from LHC for normal and inverted ordering will not cause a meaningful impact on our conclusions and with this understanding in mind, we will simply quote those in Eq.(3.5). There are other important limits on this scenario [83,[95][96][97][98] but the ones we quote are the most relevant. For a more complete discussion of the collider bounds on the type II seesaw we refer to [99].…”
Section: Searches For a Doubly Charged Scalar At The Lhcmentioning
confidence: 99%
“…This difference in the lower mass bound from LHC for normal and inverted ordering will not cause a meaningful impact on our conclusions and with this understanding in mind, we will simply quote those in Eq.(3.5). There are other important limits on this scenario [83,[95][96][97][98] but the ones we quote are the most relevant. For a more complete discussion of the collider bounds on the type II seesaw we refer to [99].…”
Section: Searches For a Doubly Charged Scalar At The Lhcmentioning
confidence: 99%
“…In the type I seesaw mechanism, heavy right-handed neutrinos lead to small neutrino masses, whereas in the type II seesaw the small scalar triplet vev justifies the small neutrino masses [59][60][61][62][63][64][65][66][67][68][69][70][71]. Notice that these mechanisms are completely different from one another but at the end have the same goal.…”
Section: Seesaw Realizations In the 2hdm-u(1)mentioning
confidence: 99%
“…Theoretical prediction for v ∼ O(10) GeV is still allowed [79]. The recent experimental upper bound is v < 25 GeV [80]. As a result, contributions from F 21,SW W and F 21,W SS to the SM-like Higgs boson decay h → Z γ can reach value of F 21,W × O(10 −2 ), which is still far from the sensitivity of the recent experiments.…”
Section: Heavy Charged Boson Effects On Higgs Decays H → Zγ In Bsmmentioning
confidence: 99%