There are two main complications in the growth process of PrCe
CuO
single crystals. The first problem is that
for different Ce concentrations, optimal growth parameters like (
) and the temperature ramp rate are different. The
Ce concentration in the crystal is found to have no direct correlation with the Ce concentration of the mixture, but is
closely related to
[24]. The optimal
must be carefully chosen to avoid a substantial Ce
concentration gradient along the
-axis direction of the crystal. The second problem is that the as-grown crystals
are not superconducting. It is generally believed that a small amount of interstitial (apical) oxygen must be removed in
order to achieve superconductivity. This was done by annealing the single crystal in an argon environment at a temperature
-
K. However, due to the limited oxygen mobility, this reduction process often results in an oxygen gradient
along the
-axis direction, especially in crystals thicker than 50
m. Increasing the annealing temperature or
reduction time evaporates the Cu atoms, causing the surface of the crystal to decompose. A solution proposed by Brinkmann
et. al. [24], and adopted by Greene's group, is to cover the entire crystal with polycrytalline
Pr
Ce
CuO
pellets of the same composition during the annealing process. The pellets act as an effective Cu
diffusion barrier. The introduction of a small amount of oxygen to the argon can speed up the process by increasing the
annealing temperature without lowering
.
Contrary to widespread belief, there are some recent experiments suggesting that O(3) apical oxygen is not removed by the reduction process [25]. The role of oxygen in the superconductivity of electron-doped cuprates is a topic of current debate.