Abstract

Inspired by the Standard Model of particle physics, we discuss a mechanism for constructing chiral, anomaly-free gauge theories. The gauge symmetries and particle content of such theories are identified using subgroups and complex representations of simple anomaly-free Lie groups, such as SO(10)SO(10) or E6E_6. We explore, using mostly SO(10)SO(10) and the 16\mathbf{16} representation, several of these "imperfect copies" of the Standard Model, including U(1)NU(1)^N theories, SU(5)⊗U(1)SU(5)\otimes U(1) theories, SU(4)⊗U(1)2SU(4)\otimes U(1)^2 theories with 4-plets and 6-plets, and chiral SU(3)⊗SU(2)⊗U(1)SU(3)\otimes SU(2)\otimes U(1). A few general properties of such theories are discussed, as well as how they might shed light on nonzero neutrino masses, the dark matter puzzle, and other phenomenologically relevant questions.

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