Signals of W′ and Z′ bosons at the LHC in the SU(3)×SO(5)×U(1) gauge-Higgs unification
- NázevTitle
- Signals of W′ and Z′ bosons at the LHC in the SU(3)×SO(5)×U(1) gauge-Higgs unificationSignals of W′ and Z′ bosons at the LHC in the SU(3)×SO(5)×U(1) gauge-Higgs unification
- Druh výsledkuResult type
- Článek v časopiseJournal article
- AutořiAuthors
- S. Funatsu, H. Hatanaka, Y. Hosotani, Y. Orikasa, N. Yamatsu
- Klíčová slovaKeywords
- Dynamical symmetry breaking models, Extensions of gauge sector, Higher-dimensional field theories, Hypothetical particle physics models
- DOIDOI
- 10.1103/PhysRevD.105.055015
- Časopis / citaceJournal / citation
- Physical Review D 105(5), 055015 (2022) · ISSN 2470-0029
- RokYear
- 2022
- JazykLanguage
- eng
- ZáznamyRecords
- ProjektProject
- Inženýrské aplikace fyziky mikrosvětaEngineering applications of microworld physics
- CitovánoCited by
- 11 (INSPIRE-HEP)
- Citace ke staženíDownload citation
- TXT · BibTeX
AbstraktAbstract
The pp→{W, W′}→lν and pp→{γ, Z, Z′}→l^+ l^− (l=e, μ) processes in the SU(3)_C×SO(5)×U(1)_X gauge-Higgs unification (GHU) models are studied, where W′ and Z′ bosons are Kaluza-Klein (KK) exited states of the electroweak gauge bosons. From the experimental data collected at the Large Hadron Collider, constraints on the KK mass scale and the Aharonov-Bohm phase are obtained. One can explore the KK mass scale in the grand unified theory inspired GHU model up to 18 TeV for the luminosity 300 fb^{−1} and 22 TeV for the luminosity 3000 fb^{−1} at √s=14 TeV.
The pp→{W, W′}→lν and pp→{γ, Z, Z′}→l^+ l^− (l=e, μ) processes in the SU(3)_C×SO(5)×U(1)_X gauge-Higgs unification (GHU) models are studied, where W′ and Z′ bosons are Kaluza-Klein (KK) exited states of the electroweak gauge bosons. From the experimental data collected at the Large Hadron Collider, constraints on the KK mass scale and the Aharonov-Bohm phase are obtained. One can explore the KK mass scale in the grand unified theory inspired GHU model up to 18 TeV for the luminosity 300 fb^{−1} and 22 TeV for the luminosity 3000 fb^{−1} at √s=14 TeV.