Pith. sign in

REVIEW 2 cited by

The Strongly Interacting WW System: Gold--Plated Modes

Not yet reviewed by Pith; the record is open.

This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.

SPECIMEN: schema-true, not a live event

T0 review · schema-true

One-sentence machine reading of the paper's core claim.

pith:XXXXXXXX · record.json · timestamp

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

The Strongly Interacting WW System: Gold--Plated Modes

classification hep-ph
keywords backgroundsbreakingelectroweaksectorsymmetryback-to-backcentralchannels
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
0 comments
read the original abstract

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.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 2 Pith papers

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

  1. Constraints on Loryons in a Two Higgs Doublet Model

    hep-ph 2026-01 conditional novelty 6.0

    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. Comment on 'Primary Dimensions'

    hep-ph 2026-07 conditional novelty 2.0

    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.