Electroweak phase transition in the economical 3-3-1 model

We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that the EWPT in the model is a sequence of two first-order phase transitions, S U ( 3 ) → S U ( 2 ) at the TeV scale and S U ( 2 ) → U ( 1 ) at the 100 GeV scale. The EWPT S U ( 3 ) → S U ( 2 ) is triggered by the new bos...

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Published inThe European physical journal. C, Particles and fields Vol. 75; no. 7; pp. 1 - 13
Main Authors Phong, Vo Quoc, Long, Hoang Ngoc, Van, Vo Thanh, Minh, Le Hoang
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.07.2015
Springer
Springer Nature B.V
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Summary:We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that the EWPT in the model is a sequence of two first-order phase transitions, S U ( 3 ) → S U ( 2 ) at the TeV scale and S U ( 2 ) → U ( 1 ) at the 100 GeV scale. The EWPT S U ( 3 ) → S U ( 2 ) is triggered by the new bosons and the exotic quarks; its strength is about 1–13 if the mass ranges of these new particles are 10 2 –10 3  GeV. The EWPT S U ( 2 ) → U ( 1 ) is strengthened by only the new bosons; its strength is about 1–1.15 if the mass parts of H 1 0 , H 2 ± and Y ± are in the ranges 10–10 2  GeV. The contributions of H 1 0 and H 2 ± to the strengths of both EWPTs may make them sufficiently strong to provide large deviations from thermal equilibrium and B violation necessary for baryogenesis.
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ISSN:1434-6044
1434-6052
DOI:10.1140/epjc/s10052-015-3550-2