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

Top quark and neutrino composite Higgs bosons

NázevTitle
Top quark and neutrino composite Higgs bosonsTop quark and neutrino composite Higgs bosons
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
A. Smetana
Klíčová slovaKeywords
electroweak symmetry breaking, flavor gauge-theory, Standard Model, mass, condensate, doublets, lhc
DOIDOI
10.1140/epjc/s10052-013-2513-8
Časopis / citaceJournal / citation
The European Physical Journal C 73(8), 2513 (2013) · ISSN 1434-6044
RokYear
2013
JazykLanguage
eng
ZáznamyRecords
ProjektProject
Příspěvek k rozšíření velké výzkumné infrastruktury evropského významuContribution of the Czech Republic to the extension of the large research infrastructure of European importance; Mezinárodní experiment ATLAS-CERNInternational Experiment ATLAS-CERN; Fundamentální experimenty ve fyzice mikrosvětaFundamental Experiments in Physics of Microworld
CitovánoCited by
16 (INSPIRE-HEP)
2013: 42014: 02015: 12016: 02017: 12018: 12019: 42020: 32021: 02022: 12023: 1
Plný text (open access)Full text (open access)
https://arxiv.org/pdf/1301.1554
Citace ke staženíDownload citation
TXT · BibTeX

AbstraktAbstract

In the context of top-quark condensation models, the top quark alone is too light to saturate the correct value of the electroweak scale by its condensate. Within the seesaw scenario the neutrinos can have their Dirac masses large enough so that their condensates can provide a significant contribution to the value of the electroweak scale. We address the question of a phenomenological feasibility of the top-quark and neutrino condensation conspiracy against the electroweak symmetry. It is mandatory to reproduce the masses of electroweak gauge bosons, the top-quark mass and the recently observed scalar mass of 125 GeV and to satisfy the upper limits on absolute value of active neutrino masses. To accomplish that we design a reasonably simplified effective model with two composite Higgs doublets. Additionally, we work with a general number N of right-handed neutrino flavor triplets participating on the seesaw mechanism. There are no experimental constraints limiting this number. The upper limit is set by the model itself. Provided that the condensation scale is of order 10(17-18) GeV and the number of right-handed neutrinos is O(100-1000), the model predicts masses of additional Higgs bosons below 250 GeV and a suppression of the top-quark Yukawa coupling to the 125 GeV particle at the similar to 60 % level of the Standard model value.

In the context of top-quark condensation models, the top quark alone is too light to saturate the correct value of the electroweak scale by its condensate. Within the seesaw scenario the neutrinos can have their Dirac masses large enough so that their condensates can provide a significant contribution to the value of the electroweak scale. We address the question of a phenomenological feasibility of the top-quark and neutrino condensation conspiracy against the electroweak symmetry. It is mandatory to reproduce the masses of electroweak gauge bosons, the top-quark mass and the recently observed scalar mass of 125 GeV and to satisfy the upper limits on absolute value of active neutrino masses. To accomplish that we design a reasonably simplified effective model with two composite Higgs doublets. Additionally, we work with a general number N of right-handed neutrino flavor triplets participating on the seesaw mechanism. There are no experimental constraints limiting this number. The upper limit is set by the model itself. Provided that the condensation scale is of order 10(17-18) GeV and the number of right-handed neutrinos is O(100-1000), the model predicts masses of additional Higgs bosons below 250 GeV and a suppression of the top-quark Yukawa coupling to the 125 GeV particle at the similar to 60 % level of the Standard model value.

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