  We discuss the gravity dual of FFLO states in strongly coupled
superconductors. The gravitational theory utilizes two U(1) gauge fields and a
scalar field coupled to a charged AdS black hole. The first gauge field couples
with the scalar sourcing a charge condensate below a critical temperature, and
the second gauge field incorporates a magnetic field that couples to spin in
the boundary theory. The scalar is neutral under the second gauge field. By
turning on a magnetic interaction between the second U(1) field and the scalar,
it is shown that, in the high-field limit, an inhomogeneous solution possesses
a higher critical temperature than the homogeneous case, giving rise to FFLO
states close to zero temperature.
