ÚTEFČVUT Ústav technické a experimentální fyziky ČVUT v PrazeInstitute of Experimental and Applied Physics, CTU in Prague

THE LHC MASS LIMITS FOR THE SU (2) (L+R) VECTOR RESONANCE TRIPLET OF A STRONG EXTENSION OF THE STANDARD MODEL

NázevTitle
THE LHC MASS LIMITS FOR THE SU (2) (L+R) VECTOR RESONANCE TRIPLET OF A STRONG EXTENSION OF THE STANDARD MODELTHE LHC MASS LIMITS FOR THE SU (2) (L+R) VECTOR RESONANCE TRIPLET OF A STRONG EXTENSION OF THE STANDARD MODEL
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
M. Gintner, J. Juráň
Klíčová slovaKeywords
Higgs boson
DOIDOI
10.5506/APhysPolB.48.1383
Časopis / citaceJournal / citation
Acta Physica Polonica B 48(8), 1383 (2017) · ISSN 0587-4254
RokYear
2017
JazykLanguage
eng
ZáznamyRecords
ProjektProject
Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.
CitovánoCited by
4 (INSPIRE-HEP)
2017: 12018: 12019: 12020: 1
Plný text (open access)Full text (open access)
https://arxiv.org/pdf/1705.04806
Citace ke staženíDownload citation
TXT · BibTeX

AbstraktAbstract

In this paper, we derive the mass exclusion limits for the hypothetical vector resonances of a strongly interacting extension of the Standard Model using the most recent upper bounds on the cross sections for various resonance production processes. The SU (2) (L+R) triplet of the vector resonances under consideration is embedded into the effective Lagrangian based on the non-linear sigma model with the 125-GeV SU (2) (L+R) scalar singlet. No direct interactions of the vector resonance to the SM fermions are assumed. We find that among eleven processes considered in this paper, only those where the vector resonances decay to WW and W Z provide the mass exclusion limit. Depending on the values of other parameters of the model, the mass limit can be as low as 1 TeV.

In this paper, we derive the mass exclusion limits for the hypothetical vector resonances of a strongly interacting extension of the Standard Model using the most recent upper bounds on the cross sections for various resonance production processes. The SU (2) (L+R) triplet of the vector resonances under consideration is embedded into the effective Lagrangian based on the non-linear sigma model with the 125-GeV SU (2) (L+R) scalar singlet. No direct interactions of the vector resonance to the SM fermions are assumed. We find that among eleven processes considered in this paper, only those where the vector resonances decay to WW and W Z provide the mass exclusion limit. Depending on the values of other parameters of the model, the mass limit can be as low as 1 TeV.

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