Higgs boson origin from a gauge symmetric theory of massive composite particles and massless $W^\pm$ and $Z^0$ bosons at the TeV scale

TL;DR

This paper proposes a gauge-symmetric theory with composite particles at high energies, explaining the Higgs boson as a composite state and predicting new phenomena at around 5.1 TeV scale.

Contribution

It introduces a gauge-symmetric four-fermion interaction framework that unifies composite particles and SM particles, connecting high-energy composite dynamics with low-energy SM phenomenology.

Findings

Composite particles emerge in the gauge symmetric phase.

The Higgs boson is a composite state from top-quark interactions.

Predicted new massive bosons at approximately 5.1 TeV.

Abstract

The ultraviolet completion is the Standard Model (SM) gauge-symmetric four-fermion couplings at the high-energy cutoff. Composite particles appear in the gauge symmetric phase in contrast with SM particles in the spontaneous symmetry-breaking phase. The critical point between the two phases is a weak first-order transition. It relates to an ultraviolet fixed point for an SM gauge symmetric theory of composite particles in the strong coupling regime. The low-energy SM realizes at an infrared fixed point in the weak coupling regime. Composite bosons dissolve into SM particles at the phase transition, and in the top-quark channel, they become a composite SM Higgs boson and three Goldstone bosons. Extrapolation of SM renormalization-group solutions to high energies implies that the gauge-symmetric theory of composite particles has a characteristic scale of about $5.1$ TeV. We discuss the phenomenological implications of composite SM Higgs boson in the gauge symmetry-breaking phase and massive composite bosons coupling to massless $W^\pm$ and $Z^0$ gauge bosons in the gauge symmetric phase.