Year: 2025
Type: article
Abstract: A bstract We demonstrate that the electroweak baryogenesis can be realized in the extended Standard Model with sequential fourth generation fermions (SM4). The solution to the coupled Dyson-Schwinger equations for the fermion and Higgs masses indicates that fourth generation quarks t ′ and b ′ with the Yukawa couplings above the threshold $$ {g}_Q^c\approx 9.1 $$ g Q c ≈ 9.1 form condensates. This critical coupling, greater than the value $$ {g}_Y^f\approx 7 $$ g Y f ≈ 7 at the ultraviolet fixed point of the renormalization-group evolution in the SM4, implies the existence of an electroweak symmetric phase at a high energy. The t ′ and b ′ Yukawa couplings evolve as the energy decreases, and exceed $$ {g}_Q^c $$ g Q c at a lower scale. The Higgs potential with the dynamical symmetry breaking effect from heavy quark condensates plus the one-loop temperature-dependent correction from the heavy scalars formed by t ′ and b ′ quarks allow the first-order phase transition characterized by the ratio ϕ c /T c ≈ 0 . 9, where ϕ c is the location of the Higgs potential minimum at the critical temperature T c . Together with the baryon number violating sphaleron interaction inherent in the Standard Model and the enhanced CP violation source from fourth generation quarks, the baryon asymmetry in the Universe can be achieved.
Source: Journal of High Energy Physics
Author: Hsiang-nan Li
Institution: Academia Sinica
Language: English
Subfield: Nuclear and High Energy Physics
Field: Physics and Astronomy
Domain: Physical Sciences
Open Access status: diamond
OpenAlex ID: W4414000656