5,379 research outputs found

    Determining VtbV_{tb} at Electron-Positron Colliders

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    Verifying Vtb≃1V_{tb} \simeq 1 is critical to test the three generation assumption of the Standard Model. So far our best knowledge of VtbV_{tb} is inferred either from the 3Γ—33\times 3 unitarity of CKM matrix or from single top-quark productions upon the assumption of universal weak couplings. The unitarity could be relaxed in new physics models with extra heavy quarks and the universality of weak couplings could also be broken if the WtbWtb coupling is modified in new physics models. In this work we propose to measure VtbV_{tb} in the process of e+eβˆ’β†’ttΛ‰e^+ e^- \to t\bar{t} without prior knowledge of the number of fermion generations or the strength of the WtbWtb coupling. Using an effective Lagrangian approach, we perform a model-independent analysis of the interactions among electroweak gauge bosons and the third generation quarks, i.e. the WtbWtb, ZttΛ‰Zt\bar{t} and ZbbΛ‰Zb\bar{b} couplings. The electroweak symmetry of the Standard Model specifies a pattern of deviations of the ZZ-tLt_L-tLt_L and WW-tLt_L-bLb_L couplings after one imposes the known experimental constraint on the ZZ-bLb_L-bLb_L coupling. We demonstrate that, making use of the predicted pattern and the accurate measurements of top-quark mass and width from the energy threshold scan experiments, one can determine VtbV_{tb} from the cross section and the forward-backward asymmetry of top-quark pair production at an {\it unpolarized} electron-positron collider.Comment: publish versio

    Combined Effect of QCD Resummation and QED Radiative Correction to W boson Observables at the Tevatron

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    A precise determination of the W boson mass at the Fermilab Tevatron requires a theoretical calculation in which the effects of the initial-state multiple soft-gluon emission and the final-state photonic correction are simultaneously included . Here, we present such a calculation and discuss its prediction on the transverse mass distribution of the W boson and the transverse momentum distribution of its decay charged lepton, which are the most relevant observables for measuring the W boson mass at hadron colliders.Comment: 10 pages, 3 Postscript figures, uses revtex4.st

    Signatures of Extra Gauge Bosons in the Littlest Higgs Model with T-parity at Future Colliders

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    We study the collider signatures of a T-odd gauge boson WHW_{H} pair production in the Littlest Higgs Model with T-parity (LHT) at Large Hadron Collider (LHC) and Linear Collider (LC). At the LHC, we search for the WHW_{H} boson using its leptonic decay, i.e. ppβ†’WH+WHβˆ’β†’AHAHβ„“+Ξ½β„“β„“β€²βˆ’Ξ½Λ‰β„“β€²pp\to W_{H}^{+}W_{H}^{-}\to A_{H}A_{H}\ell^{+}\nu_{\ell}\ell^{\prime-}\bar{\nu}_{\ell^{\prime}}, which gives rise to a collider signature of \ell^{+}\ell^{\prime-}+\met. We demonstrate that the LHC not only has a great potential of discovering the WHW_{H} boson in this channel, but also can probe enormous parameter space of the LHT. Due to four missing particles in the final state, one cannot reconstruct the mass of WHW_{H} at the LHC. But such a mass measurement can be easily achieved at the LC in the process of e+eβˆ’β†’WH+WHβˆ’β†’AHAHW+Wβˆ’β†’AHAHjjjje^{+}e^{-}\to W_{H}^{+}W_{H}^{-}\to A_{H}A_{H}W^{+}W^{-}\to A_{H}A_{H}jjjj. We present an algorithm of measuring the mass and spin of the WHW_{H} boson at the LC. Furthermore, we illustrate that the spin correlation between the WW boson and its mother particle (WHW_{H}) can be used to distinguish the LHT from other new physics models.Comment: version to appear in PRD (a few references added

    Next-to-Leading Order Corrections to Single Top Quark Production and Decay at the Tevatron: 1. s-channel Process

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    We present a study of s-channel single top quark production at the upgraded Tevatron ppˉp\bar{p} collider, including the next-to-leading order (NLO) QCD corrections to the production and the decay of the top quark. The "modified" narrow width approximation was adopted to preserve the spin of the top quark in its production and decay. We discuss the effect of the different O(αs)O(\alpha_s) contributions on the inclusive cross section as well as various kinematic distributions after imposing the relevant cuts to select s-channel single top signal events. In particular the O(αs)O(\alpha_s) decay contribution, while small in size, has a significant impact on several distributions. With the help of the best-jet algorithm to reconstruct the top quark we demonstrate that it is possible to study kinematical and spin correlations in s-channel single top events. We furthermore compare top quark spin measurements in two different basis and show how NLO corrections have to be taken into consideration in searches for the Higgs boson through W±HW^{\pm}H associated production at the Tevatron.Comment: 39 pages, 37 figure
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