2.6 Electrochemistry
of Thin Film Superconductor Electrodes
While barriers
to acquiring good electrochemistry on ceramic superconductors have
been overcome,18 the electrochemical response of redox active solution species
using bare YBa2Cu3O7-x thin
film electrodes has been problematic.21, 22 Redox active assemblies anchored on the surface, 37-40 on the other hand, have successfully been used to obtain
faradaic electron transfer reactions. One advantage that bulk
YBa2Cu3O7-x electrodes have
over thin films is that they can be mechanically resurfaced just
prior to electrochemical measurements in an inert atmosphere. This
provides a pristine surface, free of insulating corrosion products. Unfortunately,
there are no methods currently available for mechanically resurfacing
YBa2Cu3O7-x thin films to
a pristine state, though polishing and cleaving of microband edge
electrodes have proved successful.13,
14 Chemical etching of YBa2Cu3O7-x thin
films with bromine / ethanol solutions has been employed,41 but limitations of controlling the etching rate and non-uniform
etching prevent the formation of a clean uniform surface.
The electrolyte
tetraethylammonium tetrafluoroborate, Et4NBF4,
(Aldrich) was recrystallized from ethyl acetate / ethanol and vacuum
dried overnight prior to use. The compound 7,7’,8,8’-tetracyanoquinodimethane,
TCNQ, (Aldrich) was used as the redox couple. Acetonitrile was
distilled with P2O5 under N2 and
passed over activated alumina in an inert atmosphere before use. Here,
0.1 M Et4NBF4 in CH3CN was used
as electrolyte solution. Solutions containing 1mM TCNQ were also
made from the electrolyte solution. Cyclic voltammetry was accomplished
using an EG&G PAR 273 potentiostat. All electrochemical measurements
were carried out in an inert atmosphere glovebox. Thin films were
transferred from the laser ablation chamber to an inert atmosphere
with less than 2-3 minutes atmospheric exposure to prevent surface
corrosion.
Investigations
targeted YBa2Cu3O7-x thin
films since these are the most commonly researched high-temperature
superconducting thin film materials. The orientation of the thin
films can be manipulated by careful control of the deposition temperature.34 At
a temperature of 750oC, deposition of the
c-axis orientation is preferred. The a-axis orientation of YBa2Cu3O7-x is
favored when the deposition temperature is 630oC. At
temperatures between 630oC and 750oC, a mixture
of both orientations is obtained. The choice of substrates also
plays a factor in the determination of orientation.34 For
c-axis orientation, the lattice mismatches for MgO and LaAlO3 are
2.00% and 2.62%, respectively. While the
lattice mismatches for a-axis oriented thin films on MgO and LaAlO3 are
8.41% and 0.81%, respectively. There are two primary conduction
pathways in the YBa2Cu3O7-x structure. The
first conduction pathway is aligned within the a-b plane through
the copper-oxide sheets. The second pathway is along the copper
Illustration 2.5: Structural
schematic for YBa2Cu3O7-z orientations
a) a-axis b) c-axis (tilted view).
Illustration 2.6: Structural
schematic for YBa2Cu3O7-z orientations
a) a-axis b) c-axis (side view). Arrows indicate the locations
where electronic conductivity is thought to be highest within the
lattice. oxide
chains.
Illustrations
2.5(a) and 2.6(b) show that the a-axis oriented thin film positions
its copper-oxide sheets perpendicular to the electrode interface,
whereas the c-axis oriented thin film, shown in Illustrations 2.5(b)
and 2.6(b), has its copper-oxide sheets parallel to the interface. Perpendicular
alignment of the copper-oxide sheets at the surface of the electrode
may provide active sites near the electrode’s surface which promotes
electron transfer to the solution-dissolved redox species.