The spontaneous decay rate gamma of excited atomic states limits the radiat
ive force on atoms to (h) over bar k gamma/2. This bottleneck in the dissip
ative exchange of momentum between atoms and light can be overcome by coher
ent control of the momentum exchange interactions. The bichromatic force pr
ovides such control by using stimulated instead of spontaneous emission to
produce the force, while at the same time exploiting spontaneous emission t
o enable a dissipative interaction. It is implemented with two counterpropa
gating light beams, each containing two frequencies, whose phases, amplitud
es, and frequency difference are carefully chosen. We have made precise mea
surements of the extremely large magnitude and velocity range of this bichr
omatic force, and have shown that its velocity dependence near the edge of
its range is suitable for atomic beam slowing and laser cooling. Our measur
ements have corroborated various models and calculations of this bichromati
c force.