Abstract
The electrical resistance and the magnetoresistance of the ceramic superconductor Y1Ba2Cu3O9y have been precisely measured in order to extract the temperature derivative and to analyze the fluctuation regimes. The logarithmic dependence at high temperature is followed near the transition by a two-dimensional fluctuation regime in agreement with Aslamazov-Larkin theory (critical exponent λ2D=1, and a complex behavior below Tc. Our findings disprove the observation of a three-dimensional fluctuation regime near and above Tc.