Abstract
We propose a framework where a phase transition associated with a gauge symmetry breaking that occurs (not far) above the electroweak scale sets a stage for baryogenesis similar to the electroweak baryogenesis in the Standard Model. A concrete realization utilizes the breaking of SU(2)R× U(1)X→ U(1)Y. New chiral fermions charged under the extended gauge symmetry have nonzero lepton numbers, which makes the B − L symmetry anomalous. The new lepton sector contains a large flavor-dependent CP violation, similar to the Cabibbo-Kobayashi-Maskawa phase, without inducing sizable electric dipole moments of the Standard Model particles. A bubble wall dynamics associated with the first-order phase transition and SU(2)R sphaleron processes generate a lepton asymmetry, which is transferred into a baryon asymmetry via the ordinary electroweak sphaleron process. Unlike the Standard Model electroweak baryogenesis, the new phase transition can be of the strong first order and the new CP violation is not significantly suppressed by Yukawa couplings, so that the observed asymmetry can be produced. The model can be probed by collider searches for new particles and the observation of gravitational waves. One of the new leptons becomes a dark matter candidate. The model can be also embedded into a left-right symmetric theory to solve the strong CP problem.
Highlights
The question of why the Universe contains more matter than antimatter remains unsolved
As discussed in section 3.5.3, the baryon asymmetry is exponentially suppressed for the parameter regions (i)-(B) and (ii)-(B), and we focus on the parameter regions (i)-(A) and (ii)-(A)
We have proposed a new baryogenesis scenario based on a first-order phase transition associated with the spontaneous breaking of an extended gauge symmetry, SU(2)R × U(1)X → U(1)Y
Summary
The question of why the Universe contains more matter than antimatter remains unsolved. The ACME experiment [43] has ruled out a wide range of new physics with CP violation at energies even higher than what the LHC can test [44, 45] This situation drives us to explore a possibility of baryogenesis that utilizes a first order phase transition other than the electroweak one.. To generate the baryon asymmetry during the new phase transition while evading the wash-out by the electroweak sphaleron processes, the B − L symmetry must be (effectively) anomalous under the extended gauge interactions. This is achieved by introducing a new chiral sector that has baryon or lepton numbers, is charged under the SU(2)R × U(1)X , and has a structure different from the SM sector.
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