7,951 research outputs found

    Photon Polarization in the b->s gamma processes in the Left-Right Symmetric Model

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    The circular-polarization of the photon in the radiative B decays is dominantly left-handed in the Standard Model (SM), but the right-handed polarization may be enhanced in some new physics models with right-handed currents, such as the Left-Right Symmetric Model (LRSM). In this article, we investigate how large this wrong polarization could be within the allowed parameter space of the LRSM. We show that in LRSM, the right-handed polarization of the photon in the bsγb\to s\gamma processes could be largely enhanced by the WLWRW_L-W_R mixing contributions because of the helicity flip on the internal top quark line of the penguin diagrams and the enhancement by the CKM factor VtsR/VtsLV_{ts}^R/V_{ts}^L. We discuss the sensitivity of the proposed methods to determine the bsγb\to s\gamma photon polarization to the LRSM as well as their complementary role compared to the direct search of right-handed charged gauge bosons at LHC.Comment: 30pages, 5 figures, published version; references adde

    Implications on the first observation of charm CPV at LHCb

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    Very recently, the LHCb Collaboration observed the CPCP violation (CPV) in the charm sector for the first time, with ΔACPdirACP(D0K+K)ACP(D0π+π)=(1.54±0.29)×103\Delta A_{CP}^{\rm dir}\equiv A_{CP}(D^0\to K^+K^-)-A_{CP}(D^0\to \pi^+\pi^-)=(-1.54\pm0.29)\times10^{-3}. This result is consistent with our prediction of ΔACPSM=(0.571.87)×103\Delta A_{CP}^{\rm SM}=(-0.57\sim -1.87)\times 10^{-3} obtained in the factorization-assisted topological-amplitude (FAT) approach in [PRD86,036012(2012)]. It implies that the current understanding of the penguin dynamics in charm decays in the Standard Model is reasonable. Motivated by the success of the FAT approach, we further suggest to measure the D+K+Kπ+D^+\to K^+K^-\pi^+ decay, which is the next potential mode to reveal the CPV of the same order as 10310^{-3}.Comment: 10 page

    Branching ratios and direct CP asymmetries in DPPD\to PP decays

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    We propose a theoretical framework for analyzing two-body nonleptonic DD meson decays, based on the factorization of short-distance (long-distance) dynamics into Wilson coefficients (hadronic matrix elements of four-fermion operators). The parametrization of hadronic matrix elements in terms of several nonperturbative quantities is demonstrated for the DPPD\to PP decays, PP denoting a pseudoscalar meson. We consider the evolution of Wilson coefficients with energy release in individual decay modes, and the Glauber strong phase associated with the pion in nonfactorizable annihilation amplitudes, that is attributed to the unique role of the pion as a Nambu-Goldstone boson and a quark-anti-quark bound state simultaneously. The above inputs improve the global fit to the branching ratios involving the η\eta' meson, and resolves the long-standing puzzle from the D0π+πD^0\to\pi^+\pi^- and D0K+KD^0\to K^+K^- branching ratios, respectively. Combining short-distance dynamics associated with penguin operators and the hadronic parameters determined from the global fit to branching ratios, we predict direct CP asymmetries, to which the quark loops and the scalar penguin annihilation give dominant contributions. In particular, we predict ΔACPACP(K+K)ACP(π+π)=1.00×103\Delta A_{\rm CP}\equiv A_{\rm CP}(K^+K^-)-A_{\rm CP}(\pi^+\pi^-)=-1.00\times 10^{-3}, lower than the LHCb and CDF data.Comment: 17 pages, 3 figures, matches published versio

    Branching ratios and direct CP asymmetries in DPVD\to PV decays

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    We study the two-body hadronic DPVD\to PV decays, where PP (VV) denotes a pseudoscalar (vector) meson, in the factorization-assisted topological-amplitude approach proposed in our previous work. This approach is based on the factorization of short-distance and long-distance dynamics into Wilson coefficients and hadronic matrix elements of four-fermion operators, respectively, with the latter being parametrized in terms of several nonperturbative quantities. We further take into account the ρ\rho-ω\omega mixing effect, which improves the global fit to the branching ratios involving the ρ0\rho^0 and ω\omega mesons. Combining short-distance dynamics associated with penguin operators and the hadronic parameters determined from the global fit to branching ratios, we predict direct CPCP asymmetries. In particular, the direct CPCP asymmetries in the D0K0K0, K0K0D^0\to K^0\overline{K}^{*0},~\overline{K}^0K^{*0}, D+π+ρ0D^+\to\pi^+\rho^0, and Ds+K+ω, K+ϕD_s^+\to K^+\omega,~K^+\phi decays are found to be of O(103){\cal O}(10^{-3}), which can be observed at the LHCb or future Belle II experiment. We also predict the CPCP asymmetry observables of some neutral DD meson decays.Comment: 16 pages, 2 figure

    Charged lepton flavor violating Higgs decays at future e+ee^+e^- colliders

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    After the discovery of the Higgs boson, several future experiments have been proposed to study the Higgs boson properties, including two circular lepton colliders, the CEPC and the FCC-ee, and one linear lepton collider, the ILC. We evaluate the precision reach of these colliders in measuring the branching ratios of the charged lepton flavor violating Higgs decays He±μH\to e^\pm\mu^\mp, e±τe^\pm\tau^\mp and μ±τ\mu^\pm\tau^\mp. The expected upper bounds on the branching ratios given by the circular (linear) colliders are found to be B(He±μ)<1.2 (2.1)×105\mathcal{B}(H\to e^\pm\mu^\mp) < 1.2\ (2.1) \times 10^{-5}, B(He±τ)<1.6 (2.4)×104\mathcal{B}(H\to e^\pm\tau^\mp) < 1.6\ (2.4) \times 10^{-4} and B(Hμ±τ)<1.4 (2.3)×104\mathcal{B}(H\to \mu^\pm\tau^\mp) < 1.4\ (2.3) \times 10^{-4} at 95\% CL, which are improved by one to two orders compared to the current experimental bounds. We also discuss the constraints that these upper bounds set on certain theory parameters, including the charged lepton flavor violating Higgs couplings, the corresponding parameters in the type-III 2HDM, and the new physics cut-off scales in the SMEFT, in RS models and in models with heavy neutrinos.Comment: 20 pages, 2 figures (extend the CEPC study to the FCC-ee and the ILC, and to match the published version
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