5,593 research outputs found

    Search for Singly Charged Higgs in Vector Boson Scattering at the ep Colliders

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    We search for a five-plet singly charged Higgs H5±H_5^\pm in the Georgi-Machacek model at the ep colliders. The charged Higgs bosons are produced via the ZW±ZW^{\pm} fusion process pejeH5±p\, e^- \to j\, e^-\, H_5^\pm, and decay as H5±ZW±(l+l)(jj)H_5^\pm \to Z\, W^{\pm} \to (l^+ l^-)\, (jj). With a detector-level simulation at the FCC-eh and LHeC, a multi-variate analysis is performed to yield limits on the production cross section times branching ratio σ(pejeH5±)×BR(H5±ZW±)\sigma (p\, e^- \to j e^- H_5^\pm) \times {\rm BR}(H_5^\pm \to Z\, W^\pm) and on the model parameter sinθH\sin\theta_H for charged Higgs masses between 200 and 1000 GeV. The effects of electron beam polarization are also investigated.Comment: 7 pages, 6 figure

    Strong WW scattering in unitary gauge

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    A method to embed models of strong WWWW scattering in unitary gauge amplitudes is presented that eliminates the need for the effective WW approximation (EWA) in the computation of cross sections at high energy colliders.The cross sections obtained from the U-gauge amplitudes include the distributions of the final state fermions in ffffWWff \rightarrow ffWW, which cannot be obtained from the EWA. Since the U-gauge method preserves the interference of the signal and the gauge sector background amplitudes, which is neglected in the EWA, it is more accurate, especially if the latter is comparable to or bigger than the signal, as occurs for instance at small angles because of Coulomb singularities. The method is illustrated for on-shell W+W+W+W+W^+W^+ \rightarrow W^+W^+ scattering and for qqqqW+W+qq \rightarrow qqW^+W^+.Comment: 14 pages, Latex with 2 epsf-embedded postscript figure

    Prospects for the Search for a Doubly-Charged Higgs in the Left-Right Symmetric Model with ATLAS

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    We estimate the potential for observation at the LHC of a doubly charged Higgs boson, as predicted in Left-Right symmetric models. Single production by vector boson fusion, W+W+ΔL,R++W^+W^+ \to \Delta_{L,R}^{++} and pair production by the Drell-Yan process qqˉΔL,R++ΔL,Rq \bar q \to \Delta_{L,R}^{++}\Delta_{L,R}^{--} are considered. Various decay channels are investigated: dileptons, including pairs of τ\tau's, as well as $WW

    Gauge invariant formulation of strong WW scattering

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    Models of strong WWWW scattering in the ss-wave can be represented in a gauge invariant fashion by defining an effective scalar propagator that represents the strong scattering dynamics. The \sigma(qq \ra qqWW) signal may then be computed in U-gauge from the complete set of tree amplitudes, just as in the standard model, without using the effective WW approximation (EWA). The U-gauge ``transcription'' has a wider domain of validity than the EWA, and it provides complete distributions for the final state quanta, including experimentally important jet distributions that cannot be obtained from the EWA. Starting from the usual formulation in terms of unphysical Goldstone boson scattering amplitudes, the U-gauge transcription is verified by using BRS invariance to construct the complete set of gauge and Goldstone boson amplitudes in RξR_{\xi} gauge.Comment: single LaTeX file, no figures, 12 page

    Technicolor

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    Search for the radion using the ATLAS detector

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    The possibility of observing the radion using the ATLAS detector at LHC is investigated. Studies on searches for the Standard Model Higgs with the ATLAS detector are re-interpreted to obtain limits on radion decay to gamma-gamma and ZZ(*). The observability of radion decays into Higgs pairs, which subsequently decay into gamma-gamma+b-bbar or tau-tau+b-bbar is then estimate

    Single neutral heavy lepton production at electron-muon colliders

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    New heavy Majorana and Dirac neutrinos production at future electron-muon colliders are investigated. The production of a single heavy neutrino is shown to be more relevant than pair production when comparing cross sections and neutrino mass ranges. The process e±μν±We^\pm \mu^\mp \longrightarrow {\nu} \ell^{\pm} W^{\mp} is studied including on-shell and off-shell heavy neutrino effects. Distributions are calculated including hadronization effects and experimental cuts that suppress background, in order to have a clear signal for heavy neutral leptons.Comment: 4 pages, 14 jpg figures, Published Phys.Lett B494 (2000) 273-27

    New Fermions at e+^+e^- Colliders: II.~Signals and Backgrounds

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    We discuss the production, at high--energy e+^+e^- linear colliders, of new heavy fermions predicted by extensions of the Standard Model. We analyze in great details the various signals and the corresponding backgrounds for both pair production and single production in association with ordinary fermions. Concentrating on new leptons, we use a model detector for e+^+e^- collisions at a center of mass energy of 500 GeV, to illustrate the discovery potential of the Next Linear Colliders.Comment: 22 pages + 9 figures (not included: available by mail from A. Djouadi), Preprint UdeM-LPN-TH-93-15

    Dimensionless Coupling of Bulk Scalars at the LHC

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    We identify the lowest-dimension interaction which is possible between Standard Model brane fields and bulk scalars in 6 dimensions. The lowest-dimension interaction is unique and involves a trilinear coupling between the Standard Model Higgs and the bulk scalar. Because this interaction has a dimensionless coupling, it depends only logarithmically on ultraviolet mass scales and heavy physics need not decouple from it. We compute its influence on Higgs physics at ATLAS and identify how large a coupling can be detected at the LHC. Besides providing a potentially interesting signal in Higgs searches, such couplings provide a major observational constraint on 6D large-extra-dimensional models with scalars in the bulk.Comment: 20 page
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