  In the standard model of electroweak interactions the Higgs doublet is
replaced by a complex vector doublet and a real vector singlet. The gauge
symmetry is broken dynamically by a mixed condensate of the doublet and singlet
vector fields. Gauge fields get their usual standard model masses by
condensation. The new vector matter fields become massive by their gauge
invariant selfcouplings and expected to have masses of few hundred GeV.
Fermions are assigned to the gauge group in the usual manner. Fermion masses
are coming from a gauge invariant fermion-vector field interaction by a mixed
condensat, the Kobayashi-Maskawa description is unchanged. Perturbative
unitarity estimates show that the model is valid up to 2-3 TeV. It is shown
that from the new matter fields a large number of spin-one particle pairs is
expected at future high energy e^{+}e^{-} linear colliders of 500-1500 GeV. The
inclusive production cross section of new particle pairs is presented for
hadron colliders, while at the Tevatron the new particle production is too low,
at the LHC the yield is large.
