  In the vector condensate model a doublet of vector fields plays the role of
the Higgs doublet of standard model and the gauge symmetry is broken
dynamically. This results in a theory surviving the test of radiative
corrections provided the new charged and neutral vector particles B have masses
of at least several hundred GeV's. In this note we show that while at the
Tevatron the heavy B-particle production is too low, at LHC the yield is large
and, for instance, the inclusive cross section of $B^+ B^-$ pairs is 51.5
(15.3) fb at $\sqrt{s}=14$ TeV, $m_B=400(500)$ GeV.
