Abstract

We propose an extension of the Standard Model (SM) based on the $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ (3-3-1) gauge symmetry and scale invariance. Maintaining the main features of the so-called 3-3-1 models, such as the cancellation of gauge anomalies related to the number of chiral fermion generations, this model exhibits a very compact scalar sector. Only two scalar triplets and one singlet are necessary and sufficient to break the symmetries dynamically via the Coleman-Weinberg mechanism. With the introduction of an Abelian discrete symmetry and assuming a natural hierarchy among the vacuum expectation values of the neutral scalar fields, we show that all particles in the model can get phenomenologically consistent masses. In particular, most of the standard fermion masses are generated via a seesaw mechanism involving some extra heavy fermions introduced for consistency. This mechanism provides a partial solution for the fermion mass hierarchy problem in the SM. Furthermore, the simplicity of the scalar sector allows us to analytically find the conditions for the potential stability up to one-loop level and show how they can be easily satisfied. Some of the new particles, such as the scalars $H$, $H^\pm$ and all the non-SM vector bosons, are predicted to get masses around the TeV scale and, therefore, could be produced at the high-luminosity LHC. Finally, we show that the model features a residual symmetry which leads to the stability of a heavy neutral particle; the latter is expected to show up in experiments as missing energy.

Highlights

  • We propose an extension of the Standard Model (SM) based on the SUð3ÞC ⊗ SUð3ÞL ⊗ Uð1ÞX (3-3-1) gauge symmetry and scale invariance

  • The discovery of the Higgs boson [1,2], with a mass mh 1⁄4 125.38 Æ 0.14 GeV [3], and the measurements of its main properties [3,4,5,6,7] have shown that the Standard Model (SM) predictions from the spontaneous symmetry breaking mechanism—the Higgs boson couplings to the other SM fields leading to its production cross section and branching fractions—are in agreement with the current experimental observations

  • This can be interpreted as a hint that any successful new high energy theory must have in one of its low energy limits an effective scalar sector that recovers the one in the SM, with one Higgs boson

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Summary

INTRODUCTION

The discovery of the Higgs boson [1,2], with a mass mh 1⁄4 125.38 Æ 0.14 GeV [3], and the measurements of its main properties [3,4,5,6,7] have shown that the Standard Model (SM) predictions from the spontaneous symmetry breaking mechanism—the Higgs boson couplings to the other SM fields leading to its production cross section and branching fractions—are in agreement with the current experimental observations. The other vevs are due to the scalar triplets and trigger the breaking of the gauge symmetries; w breaks the 3-3-1 gauge symmetry down to the SM group, whereas v is identified with the electroweak scale so that w ≫ v ≃ 246 GeV These hierarchies among the energy scales, along with the field content in the model, lead to interesting features in the particle mass spectrum. Completing the scalar particle spectrum, there are two scalar bosons with masses proportional to vφ ≃ 103 TeV, with one of them being the scalon, i.e., the pseudo-Nambu-Goldstone of the scale invariance breakdown, and the other one, a CPodd scalar, which plays a major role in making the one-loop effective potential bounded from below At this point, it is important to emphasize that the scalar spectrum up to the TeV scale, with only three scalars h, H, and HÆ, is more compact than other popular SM extensions, such as the two-Higgs-doublet model [64].

AN OVERVIEW OF THE 3-3-1 MODEL WITH
The gauge sector
The Yukawa sector
THE MINIMAL SCALE-INVARIANT 3-3-1 MODEL
SCALAR SECTOR
FERMION SPECTRUM
Lepton masses
Quark masses
ONE-LOOP EFFECTIVE POTENTIAL
RESIDUAL SYMMETRY AND PHENOMENOLOGICAL IMPLICATIONS
VIII. CONCLUSIONS

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