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Strongly interacting dynamics and the search for new physics at the LHC

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arxiv 1601.04027 v2 pith:3NNGA6GQ submitted 2016-01-15 hep-lat hep-ph

Strongly interacting dynamics and the search for new physics at the LHC

Thomas Appelquist , Richard C. Brower , George T. Fleming , Anna Hasenfratz , Xiao-Yong Jin , Joe Kiskis , Ethan T. Neil , James C. Osborn
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Claudio Rebbi Enrico Rinaldi David Schaich Pavlos Vranas Evan Weinberg Oliver Witzel
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classification hep-lat hep-ph
keywords interactinglightmassesphysicsresonanceresultssearchspectrum
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We present results for the spectrum of a strongly interacting SU(3) gauge theory with $N_f = 8$ light fermions in the fundamental representation. Carrying out non-perturbative lattice calculations at the lightest masses and largest volumes considered to date, we confirm the existence of a remarkably light singlet scalar particle. We explore the rich resonance spectrum of the 8-flavor theory in the context of the search for new physics beyond the standard model at the Large Hadron Collider (LHC). Connecting our results to models of dynamical electroweak symmetry breaking, we estimate the vector resonance mass to be about 2 TeV with a width of roughly 450 GeV, and predict additional resonances with masses below ~3 TeV.

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Cited by 2 Pith papers

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

  1. The Roberge-Weiss transition as a probe for conformality in many-flavor QCD

    hep-lat 2026-04 unverdicted novelty 7.0

    For eight-flavor QCD the Roberge-Weiss transition temperature vanishes in the chiral limit, placing the theory inside the conformal window.

  2. SU(2) gauge theory with one and two adjoint fermions towards the continuum limit

    hep-lat 2024-07 unverdicted novelty 5.0

    Extended lattice simulations yield continuum-limit anomalous dimensions γ* = 0.170(6) for Nf=1 and γ* = 0.291(9) for Nf=2 adjoint SU(2), with chiral perturbation theory ruling out spontaneous chiral symmetry breaking.