Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/14503
Title: Proton conductivity of Y-doped BaZrO3: Pellets and thin films
Authors: Pornprasertsuk R.
Kosasang O.
Somroop K.
Horprathum M.
Limnonthakul P.
Chindaudom P.
Jinawath S.
Keywords: Bulk density
Cold isostatic press
Conduction Mechanism
Doping concentration
Film fabrication
Grain boundary conductivity
Grain boundary structure
High conductivity
Impedance spectroscopy
Oxide ion conduction
Phase present
Proton conduction
Relative bulk density
Second phase
Sintering Aid
Sputtering techniques
Surface conduction
Temperature range
Througout
Y-doped
Y-Doping
ZnO
Barium
Barium zirconate
Electric properties
Electrochemical corrosion
Electrochemical impedance spectroscopy
Grain boundaries
Grain size and shape
Pelletizing
Proton conductivity
Protons
Semiconducting silicon compounds
Sintering
Thin films
Yttria stabilized zirconia
Zinc oxide
Zirconia
Semiconductor doping
Issue Date: 2011
Abstract: Y-doped BaZrO3 (BYZ) pellets and thin films at various doping concentrations were fabricated by the cold isostatic press and 2-step sputtering techniques, respectively. By using BaCO3, 3 mol% yttria stabilized zirconia (YSZ), nano-Y2O3 powders and 1 wt% ZnO as a sintering aid, 6-40 at% BYZ pellets with no second phase and relative bulk density higher than 97% can be achieved. The highest bulk and grain boundary proton conductivities of the BYZ pellets measured by the electrochemical impedance spectroscopy (EIS) technique were obtained at 10 and 20 at% BYZ, respectively. Due to the absence of the second phase and higher bulk density, our BYZ (1 wt% ZnO) pellets show higher bulk and grain boundary conductivity than several previously reported ZnO-BYZ results. The 2-step sputtering technique for BYZ film fabrication involved two sequential steps as followed: (i) DC sputtered Y onto BaZrO3 target and (ii) RF sputtered Y-BaZrO3 target onto SiO2/Si substrate. EIS results of BYZ thin films also verify the dependence of conductivity on the Y doping concentration and reveal 102-103 times higher conductivities than those of BYZ pellets even with some YSZ phase present. The high conductivity may arise from several factors such as the surface conduction, low contamination and change of grain boundary structure. Two ionic conduction mechanisms were observed in the thin films (in air): (i) the proton conduction at T ≤ 450 °C and (ii) the oxide ion conduction at T > 450 °C. However, under humidified H2 atmosphere, the proton conduction was dominant througout the temperature range of this study. © 2011 Elsevier Masson SAS. All rights reserved.
URI: https://ir.swu.ac.th/jspui/handle/123456789/14503
https://www.scopus.com/inward/record.uri?eid=2-s2.0-79959723716&doi=10.1016%2fj.solidstatesciences.2011.04.015&partnerID=40&md5=271450dd2def248119f4baef10f93291
ISSN: 12932558
Appears in Collections:Scopus 1983-2021

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