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Chapter 2-Section 2.1
2.1 Reactivity of High-Temperature
Superconductors
The reactive
nature of high-temperature superconductors limits their use in performing
common electrochemical procedures. Here, it is particularly important
to utilize non-aqueous environments where exposure to trace amounts
of water is avoided. For example, the prototypical high-temperature
superconductor, YBa2Cu3O7-x, has been
found4 to corrode readily in water by the following reaction:
| 2YBa2Cu3O7 +
3H2O => Y2BaCuO5 + 3Ba(OH)2 +
5CuO + 1/2 O2 |
Eq. 2.1 |
| Ba(OH)2 +
CO2 => BaCO3 + H2O |
Eq. 2.2 |
An
important by-product of corrosion according to the equation above is
BaCO3. This thermodynamically stable product can precipitate
onto the surface of the electrode when water is present forming an
insulating barrier that prevents faradaic electron transfer. Acidic
solutions are also known to be detrimental to most high-temperature
superconductors. Concentrated acid solutions readily dissolve ceramic
pellets of materials such as YBa2Cu3O7-x, La1.85Sr0.15CuO4,
and Bi2Sr2CaCu2O8. Upon
dissolving YBa2Cu3O7 in an aqueous
acidic environment,5 the metal ions that constitute the lattice are liberated
to the solution according to:
| YBa2Cu3O7 +
14H+ => Y+3 + 2Ba+2 +
2Cu+2 + Cu+3 + 7H2O |
Eq. 2.3 |
Other common reagents that are known to react with YBa2Cu3O7-x are
CO and CO2. The availability of such species in the atmosphere
places severe restrictions on the environmental conditions in which
one can perform electrochemical measurements similar to that of noble
metal electrodes. This electrochemical sensitivity to corrosion has
been utilized to measure the relative reactivity of various high-temperature
superconductors.6-8 A schematic description of what happens electrochemically
upon the formation of an insulating barrier is shown in Illustration
2.1. An example of this can be seen in Figure 2.1. Measuring the
peak splitting of the oxidation and reduction of the solution redox
species was used to evaluate the surface reactivity in several environments. As
a control, a dry acetonitrile solution of 2.5 mM 7,7’,8,8’-tetracyanoquino
dimethane (TCNQ) in 0.1M tetraethylammonium tetrafluoroborate (Et4NBF4)
was used. Then, 4.5% water (by volume) was added to the same solution. Additionally,
an aqueous solution containing 2.0 mM K3Fe(CN)6 with
0.1 M NaClO4 at pH=5 was used. This information combined
with x-ray powder diffraction and scanning electron micrographs has
yielded the following reactivity trend:
YBa2Cu3O7-x > Tl2Ba2Ca2Cu3O10+x > Bi2Sr2CaCu2O8+x >
La1.85Sr0.15CuO4 > Nd1.85Ce0.15CuO4 > Nd1.85Th0.15CuO4
|
The most corrosion
resistant cuprates were Nd1.85Ce0.15CuO4 and
Nd1.85Th0.15CuO4. Unlike the other
cuprates, which have copper valences above 2.0, these materials have
copper valences of less than 2.0. This issue is believed to be a major
reason for the stability of the materials.

Illustration
2.1: Electron transfer and corresponding
voltammagrams for a pristine high-temperature superconductor electrode
surface and the same electrode surface coated by a thin film of insulator.
a) Rapid electron transfer occurs between a solution dissolved redox
couple and a pristine high-temperature superconductor electrode surface. The
corresponding voltammagram exhibits peak splitting values, DEp, close to 59 mV for this
one electron redox couple.9 b) Sluggish electron transfer occurs when thin insulating
layers collect on the surface of the high-temperature superconductor
electrode. The corresponding voltammagram has DEp values much greater than
59 mV. (Adapted from reference3)
Figure 2.1: Cyclic
voltammetry at 100 mV/s for a 2.5 mM TCNQ solution recorded at: (A)
YBa2Cu3O7-x electrode in dry CH3CN
/ 0.1 M Et4NBF4; (B) same as (A) with 4.5% water
(v/v) added to the electrolytic solution; (C) La1.85Sr0.15CuO4 electrode
in dry CH3CN / 0.1 M Et4NBF4; (D)
same as (C) with 4.5% water (v/v) added to the electrolytic solution;
(E) Nd1.85Ce0.15CuO4 electrode in
dry CH3CN / 0.1 M Et4NBF4; (F) same
as (E) with 4.5% water (v/v) added to the electrolytic solution. All
markers are equal to 10 mA. (Adapted from reference3)
All measurements place YBa2Cu3O7-x as the most reactive
of the common cuprate phases. The high reactivity of YBa2Cu3O7-x makes
it a challenge to exploit this material in the context of electrochemical
measurements.
The lattice structures for
YBa2Cu3O7-x and related cuprate
compounds possess two dimensional attributes in which high electrical
conductivity exists within the a-b plane and poor conductivity is observed
along the c-axis. There are four types of layers in YBa2Cu3O7-x: Cu(2)-O,
Cu(1)-O, Ba-O, oxygen deficient Y layer. Each of these layers is receptive
to cationic substitution. Some of these compositions have been found
to be resistant to corrosion while retaining a relatively high transition
temperature. One example is Y0.6Ca0.4Ba1.6La0.4Cu3O7-x which
has a transition temperature of 83 K and has been found10, 11 to be approximately 100 times more stable than its parent
compound.