3,486 research outputs found

    Phenomenological discriminations of the Yukawa interactions in two-Higgs doublet models with Z2Z_2 symmetry

    Get PDF
    There are four types of two-Higgs doublet models under a discrete Z2Z_2 symmetry imposed to avoid tree-level flavour-changing neutral current, i.e. type-I, type-II, type-X and type-Y models. We investigate the possibility to discriminate the four models in the light of the flavour physics data, including Bs−BˉsB_s-\bar B_s mixing, Bs,d→μ+μ−B_{s,d} \to \mu^+ \mu^-, B→τνB\to \tau\nu and Bˉ→Xsγ\bar B \to X_s \gamma decays, the recent LHC Higgs data, the direct search for charged Higgs at LEP, and the constraints from perturbative unitarity and vacuum stability. After deriving the combined constraints on the Yukawa interaction parameters, we have shown that the correlation between the mass eigenstate rate asymmetry AΔΓA_{\Delta\Gamma} of Bs→μ+μ−B_{s} \to \mu^+ \mu^- and the ratio R=B(Bs→μ+μ−)exp/B(Bs→μ+μ−)SMR={\cal B}(B_{s} \to \mu^+ \mu^-)_{exp}/ {\cal B}(B_{s} \to \mu^+ \mu^-)_{SM} could be sensitive probe to discriminate the four models with future precise measurements of the observables in the Bs→μ+μ−B_{s} \to \mu^+ \mu^- decay at LHCb.Comment: 29 pages, 4 tables, 11 figures. v3: minor corrections included, matches published version in EPJ

    Correlating the CDF WW-mass shift with the muon g−2g-2 and the b→sℓ+ℓ−b \to s \ell^+ \ell^- transitions

    Full text link
    Motivated by the latest CDF WW-mass measurement as well as the muon g−2g-2 anomaly and the discrepancies observed in b→sℓ+ℓ−b \to s \ell^+ \ell^- transitions, we propose an extension of the Standard Model (SM) with the SU(2)LSU(2)_L-singlet vector-like fermion partners that are featured by additional U(1)′U(1)^\prime gauge symmetry. The fermion partners have the same SM quantum numbers as of the right-handed SM fermions, and can therefore mix with the latter after the electroweak and the U(1)′U(1)^\prime symmetry breaking. As a result, desirable loop-level corrections to the (g−2)μ(g-2)_\mu, the WW-boson mass mWm_W and the Wilson coefficient C9C_9 in b→sμ+μ−b \to s \mu^+ \mu^- transitions can be obtained. The final allowed parameter space is also consistent with the constraints from the Z→μ+μ−Z \to \mu^+ \mu^- decay, the neutrino trident production and the LHC direct searches for the vector-like quarks and leptons.Comment: 34 pages, 15 figures, comments welcom
    • …
    corecore