Abstract
We suggest the model with the gauge group ⋯ ⊗ SU(6)⊗ SU(5) ⊗ SU(4)⊗ SU(3)⊗ SU(2)⊗ U(1). This group is the infinite continuation of the gauge group SU(4)⊗ SU(3)⊗ SU(2) ⊗ U(1) of FarhiSusskind model. The constructed model contains fermions from the fundamental representations of any SU(N) subgroups of the gauge group. In the construction of the model we use essentially the requirement that it possesses an additional discrete symmetry Z that is the continuation of the Z6 symmetry of the Standard Model. It has been found that there exists such a choice of the hypercharges of the fermions that the chiral anomaly is absent while the symmetry Z is preserved.
Original language | English |
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Pages (from-to) | 679-689 |
Number of pages | 11 |
Journal | Modern Physics Letters A |
Volume | 25 |
Issue number | 9 |
DOIs | |
State | Published - 21 Mar 2010 |
Externally published | Yes |
Keywords
- Anomaly
- Discrete symmetry
- Higgs sector
- Standard Model
- TeV physics
- Technicolor
- Unification of interaction