We calculate the Aslamazov-Larkin direct contribution to the
thermoelectric power of high-critical-temperature superconductors in one
(1D) and two (2D) dimensions, using a kinetic formalism. This extends
the results of Howson et al. limited to 3D (and that of Maki and of
Varlamov and Livanov). The singular fluctuation contribution vanishes in
2D though it was expected to behave like epsilon–1 where epsilon =
(T-T(c))/T(c). In 1D the superconductivity fluctuation contribution
diverges like (-e-epsilon–3/2)
