  We compute the electron diffusion thermopower at compressible Quantum Hall
states corresponding to even denominator fractions in the framework of the
composite fermion approach. It is shown that the deviation from the linear low
temperature behavior of the termopower is dominated by the logarithmic
temperature corrections to the conductivity and not to the thermoelectric
coefficient, although such terms are present in both quantities. The enhanced
magnitude of this effect compared to the zero field case may allow its
observation with the existing experimental techniques.
