Abstract
The relation between the autocorrelation C(t,tw) and the
integrated linear response function χ(t,tw) is studied in
the context of the large-N model for phase-ordering systems
subjected to a shear flow. In the high-temperature phase T > Tc a non-equilibrium stationary state is entered which is
characterized by a non-trivial fluctuation-dissipation relation
χ(t − tw) = 
(C(t − tw)). For quenches below
Tc the splitting of the order parameter field into two
statistically independent components, responsible for the
stationary Cst(t − tw) and aging Cag(t/tw) part
of the autocorrelation function, can be explicitly exhibited in
close analogy with the undriven case. In the regime t − tw << tw the same relation χ(t − tw) = (Cst(t − tw)) is found between the response and
Cst(t − tw), as for T > Tc. The aging part of
χ(t,tw) is negligible for tw → ∞, as
without drive, resulting in a flat χ(C) in the aging regime
t − tw >> tw.