6533b861fe1ef96bd12c4de4

RESEARCH PRODUCT

Vacuum Induced CP Violation Generating a Complex CKM Matrix with Controlled Scalar FCNC

Miguel NebotFrancisco J. BotellaGustavo C. Branco

subject

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelScalar (mathematics)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesComputer Science::Digital LibrariesHigh Energy Physics - ExperimentMinimal modelTwo-Higgs-doublet modelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QB460-466lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyHiggs bosonCP violationlcsh:QC770-798High Energy Physics::Experiment

description

We propose a viable minimal model with spontaneous CP violation in the framework of a two Higgs doublet model. The model is based on a generalised Branco–Grimus–Lavoura model with a flavoured Z2 symmetry, under which two of the quark families are even and the third one is odd. The lagrangian respects CP invariance, but the vacuum has a CP violating phase, which is able to generate a complex CKM matrix, with the rephasing invariant strength of CP violation compatible with experiment. The question of scalar mediated flavour changing neutral couplings is carefully studied. In particular we point out a deep connection between the generation of a complex CKM matrix from a vacuum phase and the appearance of scalar FCNC. The scalar sector is presented in detail, showing that the new scalars are necessarily lighter than 1 TeV. A complete analysis of the model including the most relevant constraints is performed, showing that it is viable and that it has definite implications for the observation of New Physics signals in, for example, flavour changing Higgs decays or the discovery of the new scalars at the LHC. We give special emphasis to processes like t→hc,hu, as well as h→bs,bd, which are relevant for the LHC and the ILC.

10.1140/epjc/s10052-019-7221-6http://arxiv.org/abs/1808.00493