367 research outputs found

    A Model-independent Description of New Physics effects in e+e- to t tbar

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    We study the potential of a future e+ee^+e^- collider for the search of anomalous gamma t t bar and Z t t bar couplings, assuming that CP-invariance holds. This is done in a model-independent way, considering that all six possible couplings do appear. Two experimental situations are envisaged, with and without electron beam polarization. Observability limits in the form of domains in the 6-dimensional parameter space are established. Illustrations for specific constrained models are also presented and implications for new physics searches are discussed.Comment: 26 pages and 5 figures. e-mail: [email protected]

    Spanish Wood

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    Closing dark. A seeking man. A wooden guitar Vibrating softly with what it knows— What man himself never quite grasps

    Single Top Quark Production via FCNC Couplings at Hadron Colliders

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    We calculate single top-quark production at hadron colliders via the chromo-magnetic flavor-changing neutral current couplings tˉcg\bar tcg and tˉug\bar tug. We find that the strength for the anomalous tˉcg\bar tcg (tˉug\bar tug) coupling may be probed to κc/Λ=0.092TeV1\kappa_c / \Lambda = 0.092 {TeV}^{-1} (κu/Λ=0.026TeV1\kappa_u / \Lambda = 0.026 {TeV}^{-1}) at the Tevatron with 2fb12 {fb}^{-1} of data and κc/Λ=0.013TeV1\kappa_c / \Lambda = 0.013 {TeV}^{-1} (κu/Λ=0.0061TeV1\kappa_u / \Lambda = 0.0061 {TeV}^{-1}) at the LHC with 10fb110 {fb}^{-1} of data. The two couplings may be distinguished by a comparision of the single top signal with the direct top and top decay signals for these couplings.Comment: 18 pages, 6 figures, 3 table

    Flavor changing t -> c l_1^- l_2^+ decay in the general two Higgs doublet model

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    We study the flavor changing t-> c l_1^- l_2^+ decay in the framework of the general two Higgs doublet model, the so called model III. We predict the branching ratio for l_1=\tau, l_2=\mu at the order of magnitude of BR \sim 10^{-8}.Comment: 12 Pages, 5 Figure

    Dimension-six CP-conserving operators of the third-family quarks and their effects on collider observables

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    We list all possible dimension-six CP-conserving SUc(3)×SUL(2)×UY(1)SU_c(3)\times SU_L(2) \times U_Y(1) invariant operators involving the third-family quarks which could be generated by new physics at a higher scale. Expressions for these operators after electroweak gauge symmetry breaking and the induced effective couplings WtbˉWt\bar b, XbbˉXb\bar b and XttˉXt\bar t (X=Z,γ,g,H)( X=Z,\gamma,g,H) are presented. Analytic expressions for the tree level contributions of all these operators to the observables RbR_b and AFBbA^b_{FB} at LEP I, σ(e+ebbˉ)\sigma(e^+e^-\rightarrow b\bar b) and AFBbA^b_{FB} at LEP II, σ(e+ettˉ)\sigma(e^+e^-\rightarrow t\bar t) and AFBtA_{FB}^t at the NLC, as well as σ(ppˉtbˉ+X)\sigma(p\bar p\rightarrow t\bar b+X) at the Tevatron upgrade, are provided. The effects of these operators on different electroweak observables are discussed and numerical examples presented. Numerical analyses show that in the coupling region allowed by RbR_b and AFBbA^b_{FB} at LEP I, some of the new physics operators can still have significant contributions at LEP II, the Tevatron and the NLC.Comment: 25 page

    Top-Charm Associated Production in High Energy e+ee^+e^- Collisions

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    The possibility of exploring the flavor changing neutral current tcZ/tcγtcZ/tc\gamma couplings in the production vertex for the reaction \epem\to t\bar c + \bar tc is examined. Using a model independent parameterization for the effective Lagrangian to describe the most general three-point interactions, production cross sections are found to be relatively small at LEP II, but potentially sizeable at higher energy \epem colliders. The kinematic characteristics of the signal are studied and a set of cuts are devised for clean separation of the signal from background. The resulting sensitivity to anomalous flavor changing couplings at LEP II with an integrated luminosity of 4×5004\times 500 pb1^{-1} is found to be comparable to their present indirect constraints from loop processes, while at higher energy colliders with 0.510.5-1 TeV center-of-mass energy and 50-200 fb1^{-1} luminosity, one expects to reach a sensitivity at or below the percentage level.Comment: Latex, 22 page

    Supersymmetric effects in top quark decay into polarized W-boson

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    We investigate the one-loop supersymmetric QCD (SUSY-QCD) and electroweak (SUSY-EW) corrections to the top quark decay into a b-quark and a longitudinal or transverse W-boson. The corrections are presented in terms of the longitudinal ratio \Gamma(t-->W_L b)/\Gamma(t--> W b) and the transverse ratio \Gamma(t-->W_- b)/\Gamma(t--> W b). In most of the parameter space, both SUSY-QCD and SUSY-EW corrections to these ratios are found to be less than 1% in magnitude and they tend to have opposite signs. The corrections to the total width \Gamma(t-->W b) are also presented for comparison with the existing results in the literature. We find that our SUSY-EW corrections to the total width differ significantly from previous studies: the previous studies give a large correction of more than 10% in magnitude for a large part of the parameter space while our results reach only few percent at most.Comment: Version in PRD (explanation and refs added

    Search for the Supersymmetric Partner of the Top-Quark in ppˉp \bar{p} Collisions at s=1.8TeV\sqrt{s} = 1.8 {\rm TeV}

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    We report on a search for the supersymmetric partner of the top quark (stop) produced in ttˉt \bar{t} events using 110pb1110 {\rm pb}^{-1} of ppˉp \bar{p} collisions at s=1.8TeV\sqrt{s} = 1.8 {\rm TeV} recorded with the Collider Detector at Fermilab. In the case of a light stop squark, the decay of the top quark into stop plus the lightest supersymmetric particle (LSP) could have a significant branching ratio. The observed events are consistent with Standard Model ttˉt \bar{t} production and decay. Hence, we set limits on the branching ratio of the top quark decaying into stop plus LSP, excluding branching ratios above 45% for a LSP mass up to 40 {\rm GeV/c}2^{2}.Comment: 11 pages, 4 figure

    Calibration of myocardial T2 and T1 against iron concentration.

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    BACKGROUND: The assessment of myocardial iron using T2* cardiovascular magnetic resonance (CMR) has been validated and calibrated, and is in clinical use. However, there is very limited data assessing the relaxation parameters T1 and T2 for measurement of human myocardial iron. METHODS: Twelve hearts were examined from transfusion-dependent patients: 11 with end-stage heart failure, either following death (n=7) or cardiac transplantation (n=4), and 1 heart from a patient who died from a stroke with no cardiac iron loading. Ex-vivo R1 and R2 measurements (R1=1/T1 and R2=1/T2) at 1.5 Tesla were compared with myocardial iron concentration measured using inductively coupled plasma atomic emission spectroscopy. RESULTS: From a single myocardial slice in formalin which was repeatedly examined, a modest decrease in T2 was observed with time, from mean (± SD) 23.7 ± 0.93 ms at baseline (13 days after death and formalin fixation) to 18.5 ± 1.41 ms at day 566 (p<0.001). Raw T2 values were therefore adjusted to correct for this fall over time. Myocardial R2 was correlated with iron concentration [Fe] (R2 0.566, p<0.001), but the correlation was stronger between LnR2 and Ln[Fe] (R2 0.790, p<0.001). The relation was [Fe] = 5081•(T2)-2.22 between T2 (ms) and myocardial iron (mg/g dry weight). Analysis of T1 proved challenging with a dichotomous distribution of T1, with very short T1 (mean 72.3 ± 25.8 ms) that was independent of iron concentration in all hearts stored in formalin for greater than 12 months. In the remaining hearts stored for <10 weeks prior to scanning, LnR1 and iron concentration were correlated but with marked scatter (R2 0.517, p<0.001). A linear relationship was present between T1 and T2 in the hearts stored for a short period (R2 0.657, p<0.001). CONCLUSION: Myocardial T2 correlates well with myocardial iron concentration, which raises the possibility that T2 may provide additive information to T2* for patients with myocardial siderosis. However, ex-vivo T1 measurements are less reliable due to the severe chemical effects of formalin on T1 shortening, and therefore T1 calibration may only be practical from in-vivo human studies
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