85 research outputs found

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

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    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, SU(3)β†’SU(2)SU(3) \rightarrow SU(2) at the TeV scale and SU(2)β†’U(1)SU(2) \rightarrow U(1) at the 100100 GeV scale. The EWPT SU(3)β†’SU(2)SU(3) \rightarrow SU(2) is triggered by the new bosons and the exotic quarks; its strength is about 1βˆ’131 - 13 if the mass ranges of these new particles are 102 GeVβˆ’103 GeV10^2 \,\mathrm{GeV} - 10^3 \,\mathrm{GeV}. The EWPT SU(2)β†’U(1)SU(2) \rightarrow U(1) is strengthened by only the new bosons; its strength is about 1βˆ’1.151 - 1.15 if the mass parts of H10H^0_1, H2Β±H^\pm_2 and YΒ±Y^\pm are in the ranges 10 GeVβˆ’102 GeV10 \,\mathrm{GeV} - 10^2 \,\mathrm{GeV}. The contributions of H10H^0_1 and H2Β±H^{\pm}_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.Comment: 17 pages, 9 figure
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