The Higgs sector of the SUSY reduced 3-3-1 model
arXiv:1308.0575 · doi:10.1103/PhysRevD.88.105013
Abstract
A supersymmetric version of the recently proposed reduced minimal 3-3-1 model is considered and its Higgs sector is investigated. We focus on the mass spectrum of the lightest scalars of the model. We show that Higgs mass of 125 GeV requires substantial radiative corrections. However, stops may develop small mixing and must have mass around TeV. Moreover, some soft SUSY breaking terms may lie at the electroweak scale, which alleviates some tension concerning fine tuning of the related parameters. The lightest doubly charged scalar may have mass around few hundreds of GeV, which can be probed at the LHC, while the remaining scalars of the model have masses at TeV scale.
18 pages, 5 figures, new references added and figures resolution improved
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- Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC
- Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC
- Supersymmetric reduced minimal 3-3-1 model
- Vector bileptons and the decays
- Stabilization of the Electroweak Scale in 3-3-1 Models
Cited by in corpus (12)
- Phenomenology of the 3-3-1-1 model
- Connection of , electroweak, dark matter, and collider constraints on 331 models
- Constraining Flavor Changing Interactions from LHC Run-2 Dilepton Bounds with Vector Mediators
- Lepton flavor violating decays of Standard-Model-like Higgs in 3-3-1 model with neutral lepton
- A variant of 3-3-1 model for the generation of the SM fermion mass and mixing pattern
- Excluding the Light Dark Matter Window of a 331 Model Using LHC and Direct Dark Matter Detection Data
- The Muon Anomalous Magnetic Moment in the Reduced Minimal 3-3-1 Model
- A compact 341 model at TeV scale
- Discriminating the minimal 3-3-1 models
- Chromomagnetic and chromoelectric dipole moments of quarks in the reduced 331 model
- Signal of doubly charged Higgs at colliders
- On the Higgs-like boson in the Minimal Supersymmetric 3-3-1 Model