331 model

The 331 model in particle physics offers an explanation of why there must be three families of quarks and leptons. One curious feature of the Standard Model is that the gauge anomalies cancel exactly for each of the three known quark-lepton families independently. The Standard Model thus offers no explanation of why there are three families, or indeed why there is more than one family.

The idea behind the 331 model is to extend the standard model such that all three families are required for anomaly cancellation. More specifically, in this model the three families transform differently under an extended gauge group. The perfect cancellation of the anomalies within each family is ruined, but the anomalies of the extended gauge group cancel when all three families are present. The cancellation will persist for 6, 9, ... families, so having only the three families observed in nature is the simplest possible choice of matter content.

Such a construction necessarily requires the addition of further gauge bosons and chiral fermions, which then provide testable predictions of the model in the form of elementary particles. These particles could be found experimentally at masses above the electroweak scale, which is around 100 GeV. The minimal 331 model predicts singly and doubly charged spin-one bosons, bileptons, which could show up in electron-electron scattering when it is studied at TeV energy scales and may also be produced in multi-TeV proton–proton scattering at the Large Hadron Collider.

The 331 model is an extension of the electroweak gauge symmetry from $SU(2)_W \times U(1)_Y$ to $SU(3)_L \times U(1)_X$ with $SU(2)_W \subset SU(3)_W$ and the hypercharge $Y = \beta T_8 + I X$ and the electric charge $Q=Y/2 + T_3/2$ where T₃ and T₈ are the Gell-Mann matrices of SU(3)_L and β and I are parameters of the model. The name 331 comes from the full gauge symmetry group $SU(3)_C \times SU(3)_L \times U(1)_X$.

See also

• Physics beyond the Standard Model

References

• Frampton, P.H (1992). "Chiral Dilepton Model and the Flavor Question". Physical Review Letters 69 (20): 2889–2891. Bibcode:1992PhRvL..69.2889F. doi:10.1103/PhysRevLett.69.2889. PMID 10046667.
• Pisano, F.; Pleitez, V. (1992). "An SU(3) x U(1) model for electroweak interactions". Physical Review D 46: 410–417. arXiv:hep-ph/9206242. Bibcode:1992PhRvD..46..410P. doi:10.1103/PhysRevD.46.410.
• Foot, R.; Hernandez, O.F.; Pisano, F.; Pleitez, V. (1992). "Lepton masses in an SU(3)_L x U(1)_N gauge model". Physical Review D 47 (9): 4158–4161. arXiv:hep-ph/9207264. Bibcode:1993PhRvD..47.4158F. doi:10.1103/PhysRevD.47.4158.