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    The Three Families from SU(4)A⊗SU(3)C⊗SU(2)L⊗U(1)XSU(4)_A\otimes SU(3)_C\otimes SU(2)_L\otimes U(1)_X SM-like Chiral Models

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    We give a detailed description of the model construction procedures about our new approach to the family structure of the standard model. SM-like chiral fermion spectra, largely "derivable" from the gauge anomaly constraints, are formulated in a SU(N)⊗SU(3)⊗SU(2)⊗U(1)SU(N)\otimes SU(3)\otimes SU(2)\otimes U(1) symmetry framework as an extension of the SM symmetry. The N=4N=4 case gives naturally three families as a result, with U(1)YU(1)_Y nontrivially embedded into the SU(4)A⊗U(1)XSU(4)_A\otimes U(1)_X. Such a spectrum has extra vector-like quarks and leptons. We illustrate how an acceptable symmetry breaking pattern can be obtained through a relatively simple scalar sector which gives naturally hierarchical quark mass matrices. Compatibility with various FCNC constraints and some interesting aspects of the possible phenomenological features are discussed, from a non-model specific perspective. The question of incorporating supersymmetry without putting in the Higgses as extra supermultiplet is also addressed.Comment: 43 pages RevTex, including 9 tables and 3 figure
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