Abstract

We perform lattice studies of meson mass spectra and decay constants of the $Sp(4)$ gauge theory in the quenched approximation. We consider two species of (Dirac) fermions as matter field content, transforming in the 2-index antisymmetric and the fundamental representation of the gauge group, respectively. All matter fields are formulated as Wilson fermions. We extrapolate to the continuum and massless limits, and compare to each other the results obtained for the two species of mesons. In the case of two fundamental and three antisymmetric fermions, the long-distance dynamics is relevant for composite Higgs models. This is the first lattice study of this class of theories. The global $SU(4) \times SU(6)$ symmetry is broken to the $Sp(4) \times SO(6)$ subgroup, and the condensates align with the explicit mass terms present in the lattice formulation of the theory. The main results of our quenched calculations are that, with fermions in the 2-index antisymmetric representation of the group, the masses squared and decay constant squared of all the mesons we considered are larger than the corresponding quantities for the fundamental representation, by factors that vary between $\sim$1.2 and $\sim$2.7. We also present technical results that will be useful for future lattice investigations of dynamical simulations, of composite chimera baryons, and of the approach to large $N$ in the $Sp(2N)$ theories considered. We briefly discuss their high-temperature behaviour, where symmetry restoration and enhancement are expected.

Highlights

  • In composite Higgs models (CHMs) [1,2,3], the Higgs fields, responsible for electroweak symmetry breaking, arise as pseudo-Nambu-Goldstone bosons in a more fundamental theory, addressing the little hierarchy problem of generic extensions of the Standard Model (SM) of particle physics

  • We considered the Spð4Þ gauge theory with Nf quenched Wilson-Dirac fermions Q transforming in the fundamental representation of Spð4Þ, as well as nf quenched fermions Ψ in the 2-index antisymmetric representation

  • We generated lattice ensembles consisting of gauge configurations by means of the heat bath (HB) algorithm, modified appropriately the HIRep code [80], considered meson operators OM bilinear in these fermions, and measured two-point Euclidean correlation functions of such operators on discrete lattices

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Summary

INTRODUCTION

In composite Higgs models (CHMs) [1,2,3], the Higgs fields, responsible for electroweak symmetry breaking, arise as pseudo-Nambu-Goldstone bosons (pNGBs) in a more fundamental theory, addressing the little hierarchy problem of generic extensions of the Standard Model (SM) of particle physics. [12,43] requires that the matter content consists of Nf 1⁄4 2 Dirac fields transforming in the fundamental representation of Spð2NÞ, supplemented by nf 1⁄4 3 Dirac fields transforming in the antisymmetric representation of Spð2NÞ This dynamical system is expected to yield the spontaneous breaking of the SUð4Þ × SUð6Þ global symmetry to its Spð4Þ × SOð6Þ subgroup. We consider the Spð4Þ gauge theory and treat the two species of fermions in the quenched approximation; only the gluon dynamics is captured by the lattice numerical study, but the operators used to compute the relevant correlation functions involve both types of matter fields. We explicitly write the operators relevant as sources of all the mesons in Appendix F, and in Appendix F 1 we specify the sources of PS, V and AV mesons in the SUð4Þ=Spð4Þ case, by adopting a specific choice of SUð4Þ generators and normalizations

THE MODEL
Continuum microscopic theory
The pNGB fields
EFT: Hidden local symmetry
LATTICE MODEL
Lattice definitions
Scale setting and topology
OF QUENCHED MESONS
Correlation functions
Continuum extrapolation
Quenched spectrum
GLOBAL FITS
CONCLUSIONS AND OUTLOOK
M ωjk jk ðqjT
Weakly coupling the SM gauge group
Symmetry restoration and enhancement
QiaγμPLQjCa A QiCaγμPLQjCa
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