Ginzburg–Landau theory for the time-dependent phase field in a two-dimensional d-wave superconductor

We derive a finite temperature time-dependent effective theory for the phase θ of the pairing field, which is appropriate for a 2D conducting electron system with non-retarded d-wave attraction. As for s-wave pairing the effective action contains terms with Landau damping, but their structure appears to be different from the s-wave case due to the fact that the Landau damping is determined by the quasiparticle group velocity v g , which for the d-wave pairing does not have the same direction as the non-interacting Fermi velocity v F . We show that for the d-wave pairing the Landau terms have a linear low temperature dependence and in contrast to the s-wave case are important for all finite temperatures.