The pressure effect on T-c of polycrystalline and single crystalline Y
Ba2Cu3Ox has been investigated as a function of oxygen content x by ac
-susceptibility measurements under helium pressure. In the overdoped r
egion x > 6.93 the single crystals show a negative dT(c)/dp, as expect
ed from the charge transfer model. For optimally doped samples with x
= 6.93 we find dT(c)/dp = 0.4 K/GPa which points to pressure effects o
n T-c aside from charge transfer. In the underdoped region x < 6.93 th
e dT(c)/dp values obtained from the experiment depend strongly on the
storage temperature of the sample during the experiment. When the samp
les are stored at temperatures well below 240 K throughout the entire
experiment including pressure application and pressure release, dT(c)/
dp increases to approx. 7 K/GPa at x = 6.7 but with a further decrease
of the oxygen content the dT(c)/dp drops to approx. 2 K/GPa at x = 6.
4. These effects are intrinsic to the YBa2Cu3Ox structure and can be e
xplained by considering the anisotropic structure of YBa2Cu3Ox. The de
crease of the c-axis lattice parameter results in a charge transfer to
the CuO2-planes mainly [1], whereas the compression of the a- and b-a
xis lattice parameter is known to produce different pressure effects w
hich are responsible for the peak in dT(c)/dp at x = 6.7 [2]. When pre
ssure is changed at room temperature oxygen ordering effects occur whi
ch cause a relaxation of T-c to the equilibrium value T-c(p) at this p
ressure with a time constant depending on the oxygen content x. A decr
ease of x results in a peak effect in dT(c)/dp at x = 6.7 again, which
is enhanced to approx. 12 K/GPa. If the oxygen content is decreased f
urther, dT(c)/dp first drops to 5 K/GPa at x = 6.6, but then increases
to values of more than 20 K/GPa for x < 6.42. These giant pressure ef
fects at low oxygen contents are mainly caused by a reversible T-c inc
rease (dT(c)/dp)(0) due to pressure induced oxygen ordering via oxygen
motion between unit cells.