Results are presented for the phase separation process of a binary mixture
subject to a uniform shear flow quenched from a disordered to a homogeneous
ordered phase. The kinetics of the process is described in the context of
the time-dependent Ginzburg-Landau equation with an external velocity term.
The large-n approximation is used to study the evolution of the model in t
he presence of a stationary flow and in the case of an oscillating shear. F
or stationary flow we show that the structure factor obeys a generalized dy
namical scaling. The domains grow with different typical length scales R-x
and R-perpendicular to, respectively, in the flow direction and perpendicul
arly to it. In the scaling regime R(perpendicular to)similar to t(alpha per
pendicular to) and R(x)similar to gamma(alpha x) (with logarithmic correcti
ons), gamma being the shear rate, with alpha(x)=5/4 and alpha(perpendicular
to)=1/4. The excess viscosity Delta eta after reaching a maximum relaxes t
o zero as gamma(-2)t(-3/2). Delta eta and other observables exhibit logarit
hmic-time periodic oscillations which can be interpreted as due to a growth
mechanism where stretching and breakup of domains occur cyclically. In the
case of an oscillating shear a crossover phenomenon is observed: Initially
the evolution is characterized by the same growth exponents as for a stati
onary flow. For longer times the phase-separating structure cannot align wi
th the oscillating drift and a different regime is entered with an isotropi
c growth and the same exponents as in the case without shear.