111 research outputs found

    Reduction and evaluation of two-loop graphs with arbitrary masses

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    We describe a general analytic-numerical reduction scheme for evaluating any 2-loop diagrams with general kinematics and general renormalizable interactions, whereby ten special functions form a complete set after tensor reduction. We discuss the symmetrical analytic structure of these special functions in their integral representation, which allows for optimized numerical integration. The process Z -> bb is used for illustration, for which we evaluate all the 3-point, non-factorizable g^2*alpha_s mixed electroweak-QCD graphs, which depend on the top quark mass. The isolation of infrared singularities is detailed, and numerical results are given for all two-loop three-point graphs involved in this process

    Mass and Width of a Heavy Higgs Boson

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    The gauge dependence of the Higgs-boson mass and width in the on-shell scheme of renormalization is studied in the heavy-Higgs-boson approximation. The corresponding expansions in the pole scheme are analyzed adopting three frequently employed parametrizations. The convergence properties and other theoretical features of the on-shell and pole expansions, as well as their relative merits, are discussed.Comment: 8 pages (Latex), 1 figure (Postscript

    Testing nonperturbative techniques in the scalar sector of the standard model

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    We discuss the current picture of the standard model's scalar sector at strong coupling. We compare the pattern observed in the scalar sector in perturbation theory up to two-loop with the nonperturbative solution obtained by a next-to-leading order 1/N expansion. In particular, we analyze two resonant Higgs scattering processes, ff -> H -> f'f' and ff -> H -> ZZ, WW. We describe the ingredients of the nonperturbative calculation, such as the tachyonic regularization, the higher order 1/N intermediate renormalization, and the numerical methods for evaluating the graphs. We discuss briefly the perspectives and usefulness of extending these nonperturbative methods to other theories

    The rare decay B --> X_s l^+ l^- to NNLL precision for arbitrary dilepton invariant mass

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    We present a new phenomenological analysis of the inclusive rare decay B→Xsℓ+ℓ−B \to X_s \ell^+\ell^-. In particular, we present the first calculation of the NNLL contributions due to the leading two-loop matrix elements, evaluated for arbitrary dilepton invariant mass. This allows to obtain the first NNLL estimates of the dilepton mass spectrum and the lepton forward-backward asymmetry in the high Mℓ+ℓ−2 M^2_{\ell^+ \ell^-} region, and to provide an independent check of previously published results in the low Mℓ+ℓ−2 M^2_{\ell^+ \ell^-} region. The numerical impact of these NNLL corrections in the high-mass region (Mℓ+ℓ−2>14.4GeV2 M^2_{\ell^+ \ell^-} > 14.4 GeV^2) amounts to -13% in the integrated rate, and leads to a reduction of the scale uncertainty to ±3\pm 3%. The impact of non-perturbative contributions in this region is also discussed in detail.Comment: 40 pages, 12 figures. v2: extended phenomenological discussion; results unchanged; published versio

    NLO correction to Higgs boson parameters in the 1/N expansion

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    We present the result of a calculation of the next-to-leading correction to the Higgs propagator in the 1/N expansion, where the Higgs sector is treated as an O(N) symmetric sigma-model. The results are compared with two-loop perturbation theory. The existing discrepancy between the lowest order of the 1/N expansion and perturbation theory is dramatically reduced by including the NLO in 1/N. We find a maximum effective Higgs mass of 930-980 GeV. We give an approximate relation between Higgs width and mass, which can be used for phenomenological purposes.Comment: 5 pages LaTex, 1 eps figure included. To appear in Phys.Lett.

    Perturbative and nonperturbative Higgs signals

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    We discuss the current picture of the standard Higgs sector at strong coupling and the phenomenological implications for direct searches at the LHC.Comment: Invited talk presented by A. Ghinculov at the Theory of LHC Processes meeting, 9--13 February 1998, CERN, Genev
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