The 331 Model
Authors
 DongMing Zhang (zhangdongming@…)
 Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing
 QingHong Cao (qinghongcao@…)
 Department of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing
 Collaborative Innovation Center of Qantum Matter, Beijing
 Center for High Energy Physics, Peking University, Beijing
Model Description
The 331 model is a simple extension of the SM based on the gauge group SU(3)_C x SU(3)_L x U(1)_X. There are different versions of this model which can be characterized by a parameter called beta. Models with different beta have new particles with different electric charges. But in general, they all have the same features. i) Unlike the SM that anomaly cancellation is fulfilled within each generation, the gauge anomaly is cancelled in the 331 model when considering all the generations. In particular, the number of triplets must be equal to the number of antitriplets in fermion sector, due to the nontrivial SU(3) gauge structure. The number of generations N must be a multiple of three. On the other hand, in order to ensure QCD an asymptotic free theory, the number of generations N has to be smaller than six. So N is equal to three. That explains why the SM has three generations. ii) One of the three quark generations is different from the other two, making sure that the anomaly is free, which leads to treelevel Flavour Changing Neutral Current (FCNC) through a new neutral gauge boson Z'. And if we choose the third generation of quark as a different one, the heavy top quark mass may be explained. iii) PecceiQuinn (PQ) symmetry which can solve the strong CP problem is a natural result of gauge invariance in the 331 model. Thus PQ symmetry does not suffer from quantum corrections, which means it is not a classical symmetry but a quantumlevel one. iiii) With the extension of gauge group, particles in the 331 model are richer than the SM.
References
Model Files
 331.fr: The 331 model file for general beta.
 331_1.fr: The 331 model file for beta=1/\sqrt(3).
 331_1.fr: The 331 model file for beta=+1/\sqrt(3).
 331_3.fr: The 331 model file for beta=sqrt(3).
 331_3.fr: The 331 model file for beta=+sqrt(3).
 331.nb: The Mathematica notebook to load the above model files.
Notes:
 331.fr is only used to calculate the Feynman rules for general beta, but is not used to extract the UFO or CHO model file.
 331_*.fr are used to both calculate the Feynman rules and extract the UFO or CHO model file.
 The '~' in front of some particlename in 331_1.fr and 331_1.fr represents that it's a Z2 odd neutral particle.
 The '~' makes it possible that the CHO model file extracted from 331_1.fr and 331_1.fr be implemented into the MicrOMEGAs to calculate the relic density and so on.
Attachments (6)

331.fr
(61.5 KB) 
added by zhangdongming 3 years ago.
The 331 model file for general beta

331_1.fr
(65.8 KB) 
added by zhangdongming 3 years ago.
The 331 model file for beta=1/\sqrt(3).

331_1.fr
(60.7 KB) 
added by zhangdongming 3 years ago.
The 331 model file for beta=+1/\sqrt(3).

331_3.fr
(60.8 KB) 
added by zhangdongming 3 years ago.
The 331 model file for beta=sqrt(3).

331_3.fr
(61.0 KB) 
added by zhangdongming 3 years ago.
The 331 model file for beta=+sqrt(3).

331.nb
(235.1 KB) 
added by zhangdongming 3 years ago.
The Mathematica notebook to load the above model files.
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