870 research outputs found

    Analysis of Forward-Backward and Lepton Polarization Asymmetries in B→K1ℓ+ℓ−B\to K_{1}\ell^{+}\ell^{-} Decays in the Two-Higgs-doublet Model

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    The exclusive semileptonic B→K1(1270)ℓ+ℓ−B\to K_{1}(1270) \ell^{+}\ell^{-} (ℓ=μ,τ\ell=\mu , \tau) decays are analyzed in variants of two Higgs double models (THDMs). The mass eigenstates K1(1270)K_{1}(1270) and K1(1400)K_{1}(1400) are the mixture of two axial-vector SU(3) 1P1^{1}{P}_{1} and 3P1^{3}{P}_{1} states with the mixing angle θK\theta_{K}. Making use of the form factors calculated in the Light Cone QCD approach and by taking the mixing angle θK=−34∘\theta_{K}=-34^{\circ}, the impact of the parameters of the THDMs on different asymmetries in above mentioned semileptonic BB meson decays are studied. In this context the forward-backward asymmetry and different lepton polarization asymmetries have been analyzed. We have found comprehensive effects of the parameters of the THDMs on the above mentioned asymmetries. Therefore, the precise measurements of these asymmetries at the LHC and different BB factories, for the above mentioned processes, can serve as a good tool to put some indirect constraints on the parametric space of the different versions of THDM.Comment: 25 pages, 10 figures, Accepted for Publication in PTEP. arXiv admin note: text overlap with arXiv:0804.0648 by other author

    LHCb anomaly in B→K∗μ+μ−\boldsymbol{B\to K^*\mu^+ \mu^-} optimised observables and potential of Z′\boldsymbol{Z^\prime} Model

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    Over the last few years LHCb with present energies found some discrepancies in b→sℓ+ℓ−b\to s\ell^+\ell^- FCNC transitions including anomalies in the angular observables of B→K∗μ+μ−B\to K^*\mu^+\mu^-, particularly in P5′P_5^\prime, in low dimuon mass region. Recently, these anomalies are confirmed by Belle, CMS and ATLAS. As the direct evidence of physics beyond-the-SM is absent so far, therefore, these anomalies are being interpreted as indirect hint of new physics. In this context, we study the implication of non universal family of Z′Z^\prime model to the angular observables P1,2,3P_{1,2,3}, P4,5,6′P^{\prime}_{4,5,6} and newly proposed lepton flavor universality violation observables, Q4,5Q_{4,5}, in B→K∗(→Kπ)μ+μ−B\to K^*(\to K\pi)\mu^+ \mu^- decay channel in the low dimuon mass region. To see variation in the values of these observables from their standard model values, we have chosen the different scenarios of the Z′Z^\prime model. It is found that these angular observables are sensitive to the values of the parameters of Z′Z^\prime model. We have also found that with the present parametric space of Z′Z^\prime model, the P5′P_5^\prime-anomaly could be accommodated. However, more statistics on the anomalies in the angular observables are helpful to reveal the status of the considered model and, in general, the nature of new physics.Comment: 15 pages, 5 figures. To be published in Chinese Physics

    K_1(1270)-K_1(1400) mixing and the fourth generation SM effects in B-->K_1l^+l^- decays

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    The implications of the fourth generation quarks in the B-->K_{1}(1270,1400)l^{+}l^{-} with l=mu, tau decays are studied, where the mass eigenstates K_{1}(1270) and K_{1}(1400) are the mixture of ^{1}{P}_{1} and ^{3}{P}_{1} states with the mixing angle \theta_{K}. In this context, we have studied various observables like branching ratio (BR), forward backward asymmetry (A_{FB}) and longitudinal and transverse helicity fractions (f_{L,T}) of K_{1} meson in B-->K_{1}l^{+}l^{-} decays. To study these observables, we have used the Light Cone QCD sum rules form factors and set the mixing angle \theta_{K}=-34^{o}. It is noticed that the BR is suppressed for K_{1}(1400) as a final state meson compared to that of K_{1}(1270). Same is the case when the final state leptons are tauons rather than muons. In both the situations all the above mentioned observables are quite sensitive to the fourth generation effects. Hence the measurements of these observables at LHC, for the above mentioned processes can serve as a good tool to investigate the indirect searches for the existence of fourth generation quarks.Comment: 17 pages, 14 figures, resembles with the PRD published versio

    Impact of Z′Z^{\prime} and UED parameters on different asymmetries in Bs→ϕℓ+ℓ−B_{s} \to \phi \ell^{+} \ell^{-} decays

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    A comprehensive study of the impact of new-physics on different observables for Bs→ϕℓ+ℓ−B_{s}\to \phi \ell^{+}\ell^{-} has been done. We examine the new physics models such as Z′Z^{\prime} and UED models, where the effects of new physics coming through the modification of Wilson coefficients. We have analyzed these effects through the theoretical prediction of the branching ratio, the forward-backward asymmetry, lepton polarization asymmetries and the helicity fractions of the final state meson. These all observables will definitely be measured in present and future colliders with great precision. We also pointed out that hadronic uncertainties in various physical observables are small which make them an ideal probe to establish new physics. Therefore, the measurements of these observables for the same decay would permit the detection of physics beyond the Standard Model and will also help us to distinguish between different new physics scenarios.Comment: 28 pages, 14 figure

    A New Look at the YY Tetraquarks and Ωc\Omega_c Baryons in the Diquark Model

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    We analyze the hidden charm PP-wave tetraquarks in the diquark model, using an effective Hamiltonian incorporating the dominant spin-spin, spin-orbit and tensor interactions. We compare with other PP-wave system such as PP-wave charmonia and the newly discovered Ωc\Omega_c baryons, analysed recently in this framework. Given the uncertain experimental situation on the YY states, we allow for different spectra and discuss the related parameters in the diquark model. In addition to the presently observed ones, we expect many more states in the supermultiplet of L=1L=1 diquarkonia, whose JPCJ^{PC} quantum numbers and masses are worked out, using the parameters from the currently preferred YY-states pattern. The existence of these new resonances would be a decisive footprint of the underlying diquark dynamics.Comment: Revised and extended to accommodate referee comments. Added a table and references. Accepted for publication in the EPJ
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