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This theory identifies Wilson line degrees of freedom as \"Higgs doublets.\" We consider SU(3)(c)xSU(3)(W) and SU(6) models with the compactification scale of order of a few TeV. The gauge symmetries are reduced to SU(3)(c)xSU(2)(L)xU(1)(Y) and SU(3)(c)xSU(2)(L)xU(1)(Y)xU(1), respectively, through the orbifolding boundary conditions. We estimate the one loop effective potential of \"Higgs doublets,\" and find that the electroweak breaking is realized through the radiative corrections when there are suitable numbers of bulk fields possessing the suitable representations. 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This theory identifies Wilson line degrees of freedom as \"Higgs doublets.\" We consider SU(3)(c)xSU(3)(W) and SU(6) models with the compactification scale of order of a few TeV. The gauge symmetries are reduced to SU(3)(c)xSU(2)(L)xU(1)(Y) and SU(3)(c)xSU(2)(L)xU(1)(Y)xU(1), respectively, through the orbifolding boundary conditions. We estimate the one loop effective potential of \"Higgs doublets,\" and find that the electroweak breaking is realized through the radiative corrections when there are suitable numbers of bulk fields possessing the suitable representations. 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