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The Higgs boson discovered at the LHC opened a new chapter for particle physics. Its properties need to be studied in detail to distinguish a purely standard model (SM) Higgs boson from one of many scalars in an enlarged Higgs sector. The CMS collaboration has reported a possible lepton flavor violating (LFV) signal $htomutau$, which if confirmed, implies that the Higgs sector is larger than in the SM. New physics responsible for this type of decay may, in general, also introduce other observable effects such as charge-parity (CP) violation in $hto tautau$. We study two types of models that single out the third generation and can induce large $h to mutau$ rates with different consequences for CP violation in $h to tau tau$. Predictions for the size of the CP violating couplings require knowledge of the lepton Yukawa matrices and we discuss this in the context of two different textures considering all existing constraints.
We suggest that the forward-backward asymmetry $(A_{FB})$ of the charged leptons in $ggto Htogamma Ztogamma ell^-ell^+$ process could be used to probe the CP violating $Hgamma Z$ coupling when the interference from $ggtogamma Ztogamma ell^-ell^+$ pro
We suggest that the forward-backward asymmetry $(A_{FB})$ of the charged lepton in $ggto Htogamma Ztogamma ell^-ell^+$ process could be used to probe the CP violating $Hgamma Z$ coupling when the interference from $ggtogamma Ztogamma ell^-ell^+$ proc
We study phenomenological implications of a radiative inverse seesaw dark matter model. In this model, because neutrino masses are generated at two loop level with inverse seesaw, the new physics mass scale can be as low as a few hundred GeV and the
Constraining CP-violating interactions in effective field theory (EFT) of dimension six faces two challenges. Firstly, degeneracies in the multi-dimensional space of Wilson coefficients have to be lifted. Secondly, quadratic contributions of CP-odd d
We discuss the prospects - within several models - for the observation of CP-violation (CPV) in top decays and production. The outlook looks best for t -> bW at the LHC (MSSM CPV), t -> b tau u_tau at TeV3, LHC and NLC (H^+ CPV), p p-bar -> t b-bar