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The Strongly Interacting $WW$ System: Gold--Plated Modes

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arxiv hep-ph/9306256 v1 pith:YPUNPWOM submitted 1993-06-10 hep-ph

J. Bagger , V. Barger , K. Cheung , J. Gunion , T. Han , G. A. Ladinsky , R. Rosenfeld , C.--P. Yuan This is my paper
classification hep-ph
keywords backgroundsbreakingelectroweaksectorsymmetryback-to-backcentralchannels
verification ladder T0 review T1 audit T2 compute T3 formal
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In this paper we survey the signals and backgrounds for a strongly-interacting electroweak symmetry breaking sector at hadron supercolliders in the TeV region. We study the process pp->WWX, and compute the rates for the ``gold-plated'' channels, where W^{+/-}->l^{+/-}\nu and Z -> l^+l^- (l = e,\mu), for a wide variety of models. Using a forward jet-tag, a central jet-veto and a back-to-back lepton cut to suppress the Standard Model backgrounds, we demonstrate that the SSC and LHC have substantial sensitivity to strong interactions in the electroweak symmetry breaking sector.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Constraints on Loryons in a Two Higgs Doublet Model

    hep-ph 2026-01 conditional novelty 6.0 of 10

    In a two-Higgs-doublet model, neutral singlet scalar Loryons remain viable up to about 700 GeV, while charged Loryon representations are strongly constrained by unitarity and Higgs-to-diphoton measurements.

  2. Anomalous Couplings from the Electroweak Chiral Lagrangian for Off-Shell Higgs in $gg\to Z_L Z_L$

    hep-ph 2025-07 accept novelty 6.0 of 10

    In the electroweak chiral Lagrangian, off-shell Higgs contributions to gg to Z_L Z_L at leading order reduce to two independent combinations of the anomalous couplings c_t, c_V, and c_ggh.

  3. Comment on 'Primary Dimensions'

    hep-ph 2026-07 conditional novelty 2.0 of 10

    Primary dimensions are inconsistent because their construction requires rescaling the gauge coupling in the Goldstone boson's covariant derivative, which breaks SU(2)_L gauge invariance of the Yukawa term.

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