Pith. sign in

REVIEW 1 cited by

SM EFT effects in Vector-Boson Scattering at the LHC

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 2011.07367 v4 pith:WMBJVG5B submitted 2020-11-14 hep-ph

classification hep-ph
keywords effectsbosoncurrentelectroweakfieldhl-lhcoperatorsscale
verification ladder T0 review T1 audit T2 compute T3 formal

Signed reviews

No signed human review yet.

0 comments
abstract

The assumption that the Standard Model is an Effective Field Theory (SM EFT) of a more fundamental theory at a higher, than electroweak, energy scale, implies a growth of cross-sections for electroweak Vector Boson Scattering (VBS) processes signalling the appearance of a resonance (or resonances) nearby that scale. In this article, we investigate in detail SM EFT effects from dimension-6 operators in VBS with like-sign-$W$ production in fully leptonic decay modes at the High Luminosity LHC (HL-LHC). We find that these effects are important for a handful of operators, most notably for the operator composed of three $SU(2)$ field strength tensors responsible for strong transversely polarized vector boson interactions. Current global fits on Wilson-coefficients allow for a signal immediately permissive at the HL-LHC if not accessible at the current LHC-dataset.

Discussion (0). Continue with ORCID to comment.

Forward citations

Cited by 1 Pith paper

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

  1. Can Effective $4-$Quark Operators Describe Signals of a Supersymmetric Diquark Model at the LHC?

    hep-ph 2025-06 conditional novelty 6.0 of 10

    For an RPV supersymmetric sbottom diquark model, SMEFT 4-quark operators describe LHC top-pair data only for squark masses so large that the effects are unobservable, so SMEFT bounds cannot constrain this model.

Pith tools