  We consider a minimal technicolor model in which the ordinary and technicolor
sectors are coupled by a {\it massless} scalar doublet. When technicolor
interactions become strong, the resulting technicolor condensate not only
breaks the electroweak symmetry, but also causes the scalar to develop a vacuum
expectation value. With the appropriate choice of the scalar's Yukawa
couplings, fermion masses are generated, giving us the conventional pattern of
flavor symmetry breaking. Although no explicit scalar mass term appears in the
full lagrangian of the model, the pseudoscalar states that remain in the
low-energy effective theory gain sufficient mass through technicolor
interactions to evade detection. We show that this model does not generate
unacceptably large flavor changing neutral currents, and is consistent with the
experimental constraints on oblique electroweak radiative corrections. We
determine the experimentally allowed region of the model's parameter space, and
discuss the significance of a phenomenologically viable model that has no
arbitrary dimensionful parameters. In terms of parameter counting, our model is
the simplest possible extension of the standard model.
