Abstract
Generating sufficient amount of CP violation that would account for the observed matterantimatter asymmetry in the universe is a long-standing problem in particle physics. It is a common lore that new physics beyond the Standard Model is needed for this purpose. This claim is based on earlier perturbative estimates of effective CP violation in the bosonic sector of the Standard Model induced by the quark CKM mixing as well as on the fact that the current lower limit on the Higgs boson mass rules out the possibility of a strongly first-order electroweak phase transition. We argue that within the cold electroweak baryogenesis scenario, there is still space for the baryon asymmetry to be generated solely from known electroweak physics. Sakharov’s condition of being sufficiently far off equilibrium is satisfied by coupling the Higgs boson to a new field such as the inflaton. It is this coupling rather than a thermal electroweak transition what triggers the change of the sign of the Higgs boson mass squared in the fast expanding early universe. On the Standard Model side, we further develop the program initiated by Shaposhnikov, Smit, and others. We carry out a nonperturbative calculation of the lowest effective CP-violating operator in the bosonic sector at nonzero temperature. By inspecting the temperature dependence of the effective coupling, we conclude that cold electroweak baryogenesis is viable if the electroweak phase transition in the early universe occurs at the temperature below roughly 1 GeV.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.