154 research outputs found

    Exclusive W + photon production in proton-antiproton collisions I: general formalism

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    We present a detailed computation of the fully exclusive cross section of p + antip --> W + photon + X with X = 0 and 1 jet in the framework of the factorization theorem and dimensional regularization. Order alpha-strong and photon bremsstrahlung contributions are discussed in the MS-bar mass factorization scheme. The resulting expressions are ready to be implemented numerically using Monte Carlo techniques to compute single and double differential cross sections and correlations between outgoing pairs of particles.Comment: ITP-SB-93-72, 40 pages, LateX. 3*4 figures in separate file. ([email protected]) ([email protected]

    Incorporating next-to-leading order matrix elements for hadronic diboson production in showering event generators

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    A method for incorporating information from next-to-leading order QCD matrix elements for hadronic diboson production into showering event generators is presented. In the hard central region (high jet transverse momentum) where perturbative QCD is reliable, events are sampled according to the first order tree level matrix element. In the soft and collinear regions next-to-leading order corrections are approximated by calculating the differential cross section across the phase space accessible to the parton shower using the first order (virtual graphs included) matrix element. The parton shower then provides an all-orders exclusive description of parton emissions. Events generated in this way provide a physical result across the entire jet transverse momentum spectrum, have next-to-leading order normalization everywhere, and have positive definite event weights. The method is generalizable without modification to any color singlet production process.Comment: 13 pages, 9 figure

    Amplitude Zeros in W±ZW^\pm Z Production

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    We demonstrate that the Standard Model amplitude for f1fˉ2W±Zf_1 \bar f_2 \rightarrow W^\pm Z at the Born-level exhibits an approximate zero located at cosθ=(gf1+gf2)/(gf1gf2)\cos\theta = (g^{f_1}_{-} + g^{f_2}_{-}) / (g^{f_1}_{-} - g^{f_2}_{-}) at high energies, where the gfig^{f_i}_{-} (i=1,2i=1,2) are the left-handed couplings of the ZZ-boson to fermions and θ\theta is the center of mass scattering angle of the WW-boson. The approximate zero is the combined result of an exact zero in the dominant helicity amplitudes M(±,){\cal M}(\pm,\mp) and strong gauge cancelations in the remaining amplitudes. For non-standard WWZWWZ couplings these cancelations no longer occur and the approximate amplitude zero is eliminated.Comment: 11 pages, 4 figures submitted separately as uuencoded tar-ed postscript files, FSU-HEP-940307, UCD-94-
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