Effects of Oxygen Partial Pressure and Substrate Temperature on the Structure and Morphology of Sc and Y Co-Doped ZrO<sub>2</sub> Solid Electrolyte Thin Films Prepared via Pulsed Laser Deposition

Scandium (Sc) and yttrium (Y) co-doped ZrO<sub>2</sub> (ScYSZ) thin films were prepared on a SiO<sub>2</sub>-Si substrate via pulsed laser deposition (PLD) method. In order to obtain good quality thin films with the desired microstructure, various oxygen partial pressures (&l...

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Bibliographic Details
Main Authors: Jennet R. Rabo, Makoto Takayanagi, Takashi Tsuchiya, Hideki Nakajima, Kazuya Terabe, Rinlee Butch M. Cervera
Format: Article
Language:English
Published: MDPI AG 2022-01-01
Series:Materials
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Online Access:https://www.mdpi.com/1996-1944/15/2/410
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Summary:Scandium (Sc) and yttrium (Y) co-doped ZrO<sub>2</sub> (ScYSZ) thin films were prepared on a SiO<sub>2</sub>-Si substrate via pulsed laser deposition (PLD) method. In order to obtain good quality thin films with the desired microstructure, various oxygen partial pressures (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><msub><mi>O</mi><mn>2</mn></msub></mrow></msub><mo stretchy="false">)</mo></mrow></semantics></math></inline-formula> from 0.01 Pa to 10 Pa and substrate temperatures (<i>T<sub>s</sub></i>) from 25 °C to 800 °C were investigated. X-ray diffraction (XRD) patterns results showed that amorphous ScYSZ thin films were formed at room substrate temperature while cubic polycrystalline thin films were obtained at higher substrate temperatures (<i>T<sub>s</sub></i> = 200 °C, 400 °C, 600 °C, 800 °C). Raman spectra revealed a distinct Raman shift at around 600 cm<sup>−1</sup> supporting a cubic phase. However, a transition from cubic to tetragonal phase can be observed with increasing oxygen partial pressure. Photoemission spectroscopy (PES) spectra suggested supporting analysis that more oxygen vacancies in the lattice can be observed for samples deposited at lower oxygen partial pressures resulting in a cubic structure with higher dopant cation binding energies as compared to the tetragonal structure observed at higher oxygen partial pressure. On the other hand, dense morphologies can be obtained at lower <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo> </mo><msub><mi>P</mi><mrow><msub><mi>O</mi><mn>2</mn></msub></mrow></msub></mrow></semantics></math></inline-formula> (0.01 Pa and 0.1 Pa) while more porous morphologies can be obtained at higher <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><msub><mi>O</mi><mn>2</mn></msub></mrow></msub></mrow></semantics></math></inline-formula> (1.0 Pa and 10 Pa).
ISSN:1996-1944