2005
DOI: 10.1140/epjc/s2004-02083-0
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Concerning the Landau pole in 3-3-1 models

Abstract: Some 3-3-1 models predict the existence of a non-perturbative regime at the TeV scale. We study in these models, and their supersymmetric extensions, the energy at which the non-perturbative limit and a Landau-like pole arise. An order of magnitude for the mass of the extra neutral vector boson, Z ′ , present in these models is also obtained.

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Cited by 111 publications
(126 citation statements)
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“…Such large values of M Z are potentially problematic in the 3-3-1 scenario with β = − √ 3, since the Z -boson couplings to fermions will develop a Landau pole at high enough energies. In the original model [18,19] with minimal particle content, the relevant couplings become non-perturbative for energy scales of O(5 TeV), but the turn-on of non-perturbative dynamics can be delayed by suitably enlarging the particle content of the 3-3-1 model [58,59]. To which extend such an UV deformation modifies the physics at low energies is an very interesting question, that is however beyond the scope of the present paper.…”
Section: Jhep01(2014)069mentioning
confidence: 88%
“…Such large values of M Z are potentially problematic in the 3-3-1 scenario with β = − √ 3, since the Z -boson couplings to fermions will develop a Landau pole at high enough energies. In the original model [18,19] with minimal particle content, the relevant couplings become non-perturbative for energy scales of O(5 TeV), but the turn-on of non-perturbative dynamics can be delayed by suitably enlarging the particle content of the 3-3-1 model [58,59]. To which extend such an UV deformation modifies the physics at low energies is an very interesting question, that is however beyond the scope of the present paper.…”
Section: Jhep01(2014)069mentioning
confidence: 88%
“…Demanding for integer q yields only q = −2, −1, 0, 1. As a matter of fact, the model presents a low Landau pole of a few TeV for the bounds q = 1 or −2 (see also [12]). …”
Section: Gauge Bosons and Constraintsmentioning
confidence: 99%
“…First of all, we already mentioned that in the 331 model with right-handed neutrinos the matching of the gauge couplings constants at the SU L (3) × U X (1) breaking scale requires that sin 2 θ W ≤ 3/4 [18], from which an upper bound on the bilepton mass can be derived after considering radiative corrections to sin θ W and the most recent experimental data [42]. The respective bounds is somewhat weak and contrasts with the case of the minimal 331 model, which requires that m Y 1 TeV [16,32,33] for consistency with the theoretical bound sin 2 θ W ≤ 1/4. Therefore, whereas the bileptons predicted by the minimal 331 model could be searched for via collider experiments in a near future, thereby confirming or ruling out the model, the 331 model with right-handed neutrinos would still leave open the door.…”
Section: B Numerical Evaluation and Discussionmentioning
confidence: 99%