Abstract

Composite Higgs models must exhibit very different dynamics from quantum chromodynamics (QCD) regardless whether they describe the Higgs boson as a dilatonlike state or a pseudo-Nambu-Goldstone boson. Large separation of scales and large anomalous dimensions are frequently desired by phenomenological models. Mass-split systems are well-suited for composite Higgs models because they are governed by a conformal fixed point in the ultraviolet but are chirally broken in the infrared. In this work we use lattice field theory calculations with domain wall fermions to investigate a system with four light and six heavy flavors. We demonstrate how a nearby conformal fixed point affects the properties of the four light flavors that exhibit chiral symmetry breaking in the infrared. Specifically we describe hyperscaling of dimensionful physical quantities and determine the corresponding anomalous mass dimension. We obtain $y_m=1+\gamma^*= 1.47(5)$ suggesting that $N_f=10$ lies inside the conformal window. Comparing the low energy spectrum to predictions of dilaton chiral perturbation theory, we observe excellent agreement which supports the expectation that the 4+6 mass-split system exhibits near-conformal dynamics with a relatively light $0^{++}$ isosinglet scalar.

Highlights

  • For gauge theories describing the Higgs sector as a composite structure, experimental observations imply that a large separation of scales between the electroweak scale (IR) and new ultraviolet physics (UV) [4,5,6,7,8,9,10,11] is required

  • We show that physical masses exhibit hyperscaling and determine the universal mass scaling dimension of the corresponding Nf 1⁄4 10 system ym 1⁄4 1 þ γ⋆m 1⁄4 1.47ð5Þ

  • This value is smaller than expected for a theory near the edge of the conformal window suggesting that Nf 1⁄4 9 or 8 flavor models could be closer to the sill of the conformal window

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Summary

INTRODUCTION

Experiments have discovered a 125 GeV Higgs boson [1,2,3] but so far, up to a few TeV, no direct signs of physics. Theories with a large separation of scales part company from QCD, exhibiting a “walking” gauge coupling [12,13,14], and providing a dynamical mechanism for electroweak (EW) symmetry breaking. By choosing a theory with four fermions in the light, chirally broken sector, our simulations can directly be related to existing models extending the SM with a new strongly interacting sector [41,42,43] In these models the Higgs boson is a pseudo-Nambu-Goldstone boson (pNGB) of the new strong sector [41,42,44,45,46]. We explore this new, strongly coupled theory by performing large scale numerical lattice-field-theory simulations. Preliminary results have been reported in [56,57]

NUMERICAL SIMULATIONS
HYPERSCALING
LOW ENERGY EFFECTIVE DESCRIPTION
CONCLUSION
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