NARROW-RESONANCE IN E(-)E(-) SCATTERING DUE TO ADDITIONAL GAUGE BOSON

It now appears phenomenologically that the third family may be essenti ally different from the first two. Particularly the high value of the top quark mass suggests a special role. In the standard model all thre e families are treated similarly [becoming exactly the same at asympto tically high energies] so I need to extend the model to accommodate th e goal of a really different third family. In this article I describe one such viable extension, the 331 model which predicts bileptonic gau ge bosons.