Systematic measurements of the in-plane fluctuation magnetoconductivity in
a YBa2Cu3O7 single crystal are presented. Fields between 0 and 14 T were ap
plied either parallel or perpendicular to the Cu-O atomic planes. The data
reveal the occurrence of a large Gaussian regime in the normal phase. Far a
bove T-c, the mean-held fluctuation spectrum is effectively two dimensional
. Decreasing the temperature towards T-c, a crossover to a three-dimensiona
l (3D) Gaussian regime is seen at low applied fields. The analysis of these
results allows the estimation of the coherence length perpendicular and pa
rallel to the Cu-O planes, and reveals that superconductivity in YBa2Cu3O7
is characterized by a double planar periodicity. The c lattice parameter is
the relevant periodicity length of the 2D behavior, whereas the smallest d
istance between the double Cu-O layers plays an important role in the 3D fl
uctuation spectrum. In fields above 5 T applied parallel to the c axis, the
fluctuation magnetoconductivity scales as predicted by the 3D lowest-Landa
u-level approximation of the Ginzburg-Landau theory. Very close to T-c, and
for quite low values of the applied field, the results clearly show the oc
currence of a genuine critical regime, where the exponent is consistent wit
h the predictions of the full dynamic 3D XY universality class. Still close
r to T-c, evidence is found for a fluctuation regime beyond 3D XY scaling.
This new scaling raises the interesting possibility for the ultimate weakly
first-order character of the superconducting transition in YBa2Cu3O7-delta
. The whole set of data is condensed on H-T diagrams, which display the reg
ions of stability for the observed fluctuation regimes, in fields oriented
parallel or perpendicular to the Cu-O layers.