4.8 Article

On Proton Conductivity in Porous and Dense Yttria Stabilized Zirconia at Low Temperature

Journal

ADVANCED FUNCTIONAL MATERIALS
Volume 23, Issue 15, Pages 1957-1964

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/adfm.201202020

Keywords

yttria-stabilized-zirconia; proton conductivity; thin films; porosity; nanoctystallinity

Funding

  1. Electron Microscopy of ETH Zurich (EMEZ)
  2. Swiss National Foundation (SNF) [CRSI22-126830]
  3. Korean-Swiss Science and Technology Cooperation
  4. International Institute for Carbon Neutral Energy Research (WPI-I2CNER)
  5. World Premier International Research Center Initiative (WPI), MEXT, Japan
  6. Swiss National Science Foundation (SNF) [CRSI22_126830] Funding Source: Swiss National Science Foundation (SNF)

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The electrical conductivity of dense and nanoporous zirconia-based thin films is compared to results obtained on bulk yttria stabilized zirconia (YSZ) ceramics. Different thin film preparation methods are used in order to vary grain size, grain shape, and porosity of the thin films. In porous films, a rather high conductivity is found at room temperature which decreases with increasing temperature to 120 degrees C. This conductivity is attributed to proton conduction along physisorbed water (Grotthuss mechanism) at the inner surfaces. It is highly dependent on the humidity of the surrounding atmosphere. At temperatures above 120 degrees C, the conductivity is thermally activated with activation energies between 0.4 and 1.1 eV. In this temperature regime the conduction is due to oxygen ions as well as protons. Proton conduction is caused by hydroxyl groups at the inner surface of the porous films. The effect vanishes above 400 degrees C, and pure oxygen ion conductivity with an activation energy of 0.9 to 1.3 eV prevails. The same behavior can also be observed in nanoporous bulk ceramic YSZ. In contrast to the nanoporous YSZ, fully dense nanocrystalline thin films only show oxygen ion conductivity, even down to 70 degrees C with an expected activation energy of 1.0 +/- 0.1 eV. No proton conductivity through grain boundaries could be detected in these nanocrystalline, but dense thin films.

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