This report summarises the physics opportunities for the study of Higgs bosons and the dynamics of electroweak symmetry breaking at the 100 TeV pp collider.
The right-handed neutrinos within the type-I seesaw mechanism can induce large radiative corrections to the Higgs mass, and naturalness arguments can then be used to set limits on their mass scale and Yukawa couplings. Driven by minimality, we consider the presence of two degenerate right-handed neutrinos. We compare the limits from naturalness with the ones from the stability of the electroweak vacuum and from lepton flavor violation. Implications from neutrinoless double beta decay are also discussed and renormalization effects for the light neutrino parameters are presented. Adding small perturbations to the degenerate heavy neutrino spectrum allows for successful leptogenesis.
In this paper we consider the generation of naturally small neutrino masses from a dimension-7 operator. Such a term can arise in the presence of a scalar quadruplet and a pair of vectorlike fermion triplets and enables one to obtain small neutrino masses through the TeV scale linear seesaw mechanism. We study the phenomenology of the charged scalars of this model, in particular, the multilepton signatures at the Large Hadron Collider. Of special importance is the presence of the same-sign-tri-lepton signatures originating from the triply charged scalars. The Standard Model background for such processes is small, and hence this is considered as a confirming evidence of new physics. We also looked for events with three, four, five, and six leptons that have negligible contamination from the Standard Model. We further point out the spectacular lepton flavor violating the four-lepton signal that can be the hallmark for these types of models. We also compute the added contributions in the rate for the Standard Model Higgs decaying to two photons via the charged scalars in this model.
The charged Higgs boson sector of the Minimal Manifest Left-Right Symmetric model (MLRSM) is investigated in the context of LHC discovery search for new physics beyond Standard Model. We discuss and summarise the main processes within MLRSM where heavy charged Higgs bosons can be produced at the LHC. We explore the scenarios where the amplified signals due to relatively light charged scalars dominate against heavy neutral Z 2 and charged gauge W 2 as well as heavy neutral Higgs bosons signals which are dumped due to large vacuum expectation value v R of the right-handed scalar triplet. Consistency with FCNC effects implies masses of two neutral Higgs bosons A 0 1 , H 0 1 to be at least of 10 TeV order, which in turn implies that in MLRSM only three of four charged Higgs bosons, namely H ±± 1,2 and H ± 1 , can be simultaneously light. In particular, production processes with one and two doubly charged Higgs bosons are considered. We further incorporate the decays of those scalars leading to multi lepton signals at the LHC. Branching ratios for heavy neutrino N R , W 2 and Z 2 decay into charged Higgs bosons are calculated. These effects are substantial enough and cannot be neglected. The tri-and four-lepton final states for different benchmark points are analysed. Kinematic cuts are chosen in order to strength the leptonic signals and decrease the Standard Model (SM) background. The results are presented using di-lepton invariant mass and lepton-lepton separation distributions for the same sign (SSDL) and opposite sign (OSDL) di-leptons as well as the charge asymmetry are also discussed. We have found that for considered MLRSM processes tri-lepton and four-lepton signals are most important for their detection when compared to the SM background. Both of the signals can be detected at 14 TeV collisions at the LHC with integrated luminosity at the level of 300 fb −1 with doubly charged Higgs bosons up to approximately 600 GeV. Finally, possible extra contribution of the charged MLRSM scalar particles to the measured Higgs to di-photon (H 0 0 → γγ) decay is computed and pointed out.
Production and decays of doubly charged Higgs bosons at the LHC and future hadron colliders triggered by vector boson fusion mechanism are discussed in the context of the Minimal Left-Right Symmetric Model. Our analysis is based on the Higgs boson mass spectrum compatible with available constraints which include FCNC effects and vacuum stability of the scalar potential. Though the parity breaking scale vR is large (∼ few TeV) and scalar masses which contribute to FCNC effects are even larger, consistent Higgs boson mass spectrum still allows us to keep doubly charged scalar masses below 1 TeV which is an interesting situation for LHC and future FCC colliders. We have shown that the allowed Higgs bosons mass spectrum constrains the splittingsAssuming that doubly charged Higgs bosons decay predominantly into a pair of same sign charged leptons through the process pp → H ±± 1/2 H ∓∓ 1/2 jj → ℓ ± ℓ ± ℓ ∓ ℓ ∓ jj, we find that for LHC operating at √ s = 14 TeV with an integrated luminosity at the level of 3000 fb −1 (HL-LHC), there is practically no chance to detect such particles at the reasonable significance level through this channel. However, at 33 TeV HE-LHC and (or) 100 TeV FCC-hh a wide region opens up for exploring the doubly charged Higgs boson mass spectrum. In FCC-hh, doubly charged Higgs bosons mass up to 1 TeV can be easily probed.
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