Constraints on the SU(3) electroweak model

We consider a recent proposal by Dimopoulos and Kaplan to embed the electroweak SU(2)LxU(1)Y into a larger group SU(3)WxSU(2)xU(1) at a scale above a TeV. This idea is motivated by the prediction for the weak mixing angle sin2θW=1/4, which naturally appears in these models so long as the gauge couplings of the high energy SU(2) and U(1) groups are moderately large. The extended gauge dynamics results in new effective operators that contribute to four-fermion interactions and Z pole observables. We calculate the corrections to these electroweak precision observables and carry out a global fit of the new physics to the data. For SU(2) and U(1) gauge couplings larger than 1, we find that the 95% C.L. lower bound on the matching (heavy gauge boson mass) scale is 11 TeV. We comment on the fine-tuning of the high energy parameters needed to allow matching scales above our bounds. The remnants of SU(3)W breaking include multi-TeV SU(2)L doublets with electric charge (±2,±1). The lightest charged gauge boson is stable, leading to cosmological difficulties