8 research outputs found

    Doubly charged Higgs from ee-γ\gamma scattering in the 3-3-1 Model

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    We studied the production and signatures of doubly charged Higgs bosons in the process γe−→H−−E+\gamma e^- \rightarrow H^{--}E^+, where E+E^+ is a heavy lepton, at the e−e+e^-e^+ International Linear Collider (ILC) and CERN Linear Collider (CLIC). The intermediate photons are given by the Weizsa¨\ddot{a}cker-Williams and laser backscattering distributions. We found that significant signatures are obtained by bremsstrahlung and backward Comptom scattering of laser. A clear signal can be obtained for doubly charged Higgs bosons, doubly charged gauge bosons and heavy leptons

    Pseudo Goldstone Bosons Phenomenology in Minimal Walking Technicolor

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    We construct the non-linear realized Lagrangian for the Goldstone Bosons associated to the breaking pattern of SU(4) to SO(4). This pattern is expected to occur in any Technicolor extension of the standard model featuring two Dirac fermions transforming according to real representations of the underlying gauge group. We concentrate on the Minimal Walking Technicolor quantum number assignments with respect to the standard model symmetries. We demonstrate that for, any choice of the quantum numbers, consistent with gauge and Witten anomalies the spectrum of the pseudo Goldstone Bosons contains electrically doubly charged states which can be discovered at the Large Hadron Collider.Comment: 25 pages, 5 figure

    Static quantities of the W boson in the SU_L(3) X U_X(1) model with right-handed neutrinos

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    The static electromagnetic properties of the WW boson, Δκ\Delta \kappa and ΔQ\Delta Q, are calculated in the SU_L(3)} \times U_X(1) model with right-handed neutrinos. The new contributions from this model arise from the gauge and scalar sectors. In the gauge sector there is a new contribution from a complex neutral gauge boson Y0Y^0 and a singly-charged gauge boson Y±Y^\pm. The mass of these gauge bosons, called bileptons, is expected to be in the range of a few hundreds of GeV according to the current bounds from experimental data. If the bilepton masses are of the order of 200 GeV, the size of their contribution is similar to that obtained in other weakly coupled theories. However the contributions to both ΔQ\Delta Q and Δκ\Delta \kappa are negligible for very heavy or degenerate bileptons. As for the scalar sector, an scenario is examined in which the contribution to the WW form factors is identical to that of a two-Higgs-doublet model. It is found that this sector would not give large corrections to Δκ\Delta \kappa and ΔQ\Delta Q.Comment: New material included. Final version to apppear in Physical Review

    Determination of Leptoquark Properties in Polarized eγe\gamma Collisions

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    We study leptoquark production using polarized eγe\gamma colliders for the center of mass energies s=500\sqrt s=500~GeV and 1~TeV. We show that using polarization asymmetries the ten different types of leptoquarks listed by Buchm\"uller, R\"uckl and Wyler can be distinquished from one another for leptoquark masses essentially up to the kinematic limit of the respective colliders. Thus, if a leptoquark were discovered an eγe\gamma collider could play a crucial role in determining its origins.Comment: 10 pages (plus 10 postscript figures submitted separately), OCIP/C 94-

    Resolved Photon Contributions to Leptoquark Production in e+e−e^+ e^- and eγe\gamma Collision

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    We calculate the resolved photon contribution to leptoquark production at eγe\gamma colliders for the center of mass energies s=500\sqrt s=500~GeV and 1~TeV. We also calculate the resolved photon contribution to leptoquark production at e+e−e^+ e^- colliders for the center of mass energies s=1\sqrt{s} = 1~and~2~TeV. In both cases we find that these contributions are considerably larger than the standard contributions considered in the literature.Comment: 9 pages (5 postscript figures in separate uuencoded file), OCIP/C 93-1
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