1. Collider signatures of vector-like fermions from a flavor symmetric model
- Author
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Cesar Bonilla, A. E. Cárcamo Hernández, João Gonçalves, Felipe F. Freitas, António P. Morais, and R. Pasechnik
- Subjects
Nuclear and High Energy Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,QC770-798 ,Computer Science::Digital Libraries ,01 natural sciences ,High Energy Physics - Experiment ,vector-like quarks ,High Energy Physics - Phenomenology ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,Hadron-Hadron scattering (experiments) ,Nuclear and particle physics. Atomic energy. Radioactivity ,Beyond Standard Model ,0103 physical sciences ,Computer Science::Mathematical Software ,High Energy Physics::Experiment ,Vector-like quarks ,010306 general physics - Abstract
We propose a model with two Higgs doublets and several $SU(2)$ scalar singlets with a global non-Abelian flavor symmetry $\mathcal{Q}_6\times\mathcal{Z}_2$. This discrete group accounts for the observed pattern of fermion masses and mixing angles after spontaneous symmetry breaking. In this scenario only the third generation of fermions get their masses as in the Standard Model (SM). The masses of the remaining fermions are generated through a seesaw-like mechanism. To that end, the matter content of the model is enlarged by introducing electrically charged vector-like fermions (VLFs), right handed Majorana neutrinos and several SM scalar singlets. Here we study the processes involving VLFs that are within the reach of the Large Hadron Collider (LHC). We perform collider studies for vector-like leptons (VLLs) and vector-like quarks (VLQs), focusing on double production channels for both cases, while for VLLs single production topologies are also included. Utilizing genetic algorithms for neural network optimization, we determine the statistical significance for a hypothetical discovery at future LHC runs. In particular, we show that we can not safely exclude VLLs for masses greater than $200~\mathrm{GeV}$. For VLQ's in our model, we show that we can probe their masses up to 3.8 TeV, if we take only into account the high-luminosity phase of the LHC. Considering Run-III luminosities, we can also exclude VLQs for masses up to $3.4~\mathrm{TeV}$. We also show how the model with predicted VLL masses accommodates the muon anomalous magnetic moment., Comment: 32 pages,16 figures. Additional references and discussion. Matches version to be published in JHEP
- Published
- 2021
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