2007
DOI: 10.1016/j.stam.2007.09.008
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Nanoionics phenomenon in proton-conducting oxide: Effect of dispersion of nanosize platinum particles on electrical conduction properties

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Cited by 13 publications
(12 citation statements)
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“…In case of the “Ohmic” BZCY/Pd junctions, the [normalHnormali·] in the interfacial region of BZCY electrolyte is not depleted according to the hole–proton equilibrium because Ohmic contact accepts relatively high [h • ] in the interfacial region (Figure c,e), whereas allowable [normalHnormali·] in the interfacial region of the Schottky‐type junction would be much lower than that of the Ohmic contact because of lowering [h • ] in the interfaces (Figure d,f). In fact, it has been reported that the SrZr 0.9 Y 0.1 O 3 /Pd junction which forms Schottky‐type potential barrier with wide depletion layer at the interface shows lessened conductivity because the proton concentrations in the interfacial layer becomes smaller than those of the SrZr 0.9 Y 0.1 O 3 bulk . These imply that the proton incorporation via “Ohmic” BZCY/Pd junction is much faster than that via Schottky‐type junction due to the relatively large acceptable concentrations of hydrogen defects ([normalHnormali·]) in the interfacial region (Figure e).…”
Section: Discussionmentioning
confidence: 99%
“…In case of the “Ohmic” BZCY/Pd junctions, the [normalHnormali·] in the interfacial region of BZCY electrolyte is not depleted according to the hole–proton equilibrium because Ohmic contact accepts relatively high [h • ] in the interfacial region (Figure c,e), whereas allowable [normalHnormali·] in the interfacial region of the Schottky‐type junction would be much lower than that of the Ohmic contact because of lowering [h • ] in the interfaces (Figure d,f). In fact, it has been reported that the SrZr 0.9 Y 0.1 O 3 /Pd junction which forms Schottky‐type potential barrier with wide depletion layer at the interface shows lessened conductivity because the proton concentrations in the interfacial layer becomes smaller than those of the SrZr 0.9 Y 0.1 O 3 bulk . These imply that the proton incorporation via “Ohmic” BZCY/Pd junction is much faster than that via Schottky‐type junction due to the relatively large acceptable concentrations of hydrogen defects ([normalHnormali·]) in the interfacial region (Figure e).…”
Section: Discussionmentioning
confidence: 99%
“…The potential of nanoionics to create a super-ionic composite conductor represents a particularly fascinating and practical application. This can be created by engineering an ionic composite with appropriately spaced metal nanoparticles (NPs) to create a percolating space charge region that acts as a fast pathway for ion conduction [7][8][9][10][11]. One key issue with this approach is the need to prevent agglomeration of the metal NPs during the processing of the super-ionic composite.…”
Section: Introductionmentioning
confidence: 99%
“…Cerversa et al [46] have compared the protonic conduction of nanostructured BaZr 0.8 Y 0.2 O 3 − δ and found a contradictory effect when comparing with the overall conduction for the bulk conductivity of BaZr 0.8 Y 0.2 O 3 − δ which was already reported by Kreuer [85]. Matsumoto et al [120] made an experimental observation and established a marked change in the electrical properties in the proton conductor SrZr 0.9 Y 0.1 O 3−δ by dispersing fine platinum particles. An experimental comparative study was made with pure SrZr 0.9 Y 0.1 O 3−δ and Pt/ SrZr 0.9 Y 0.1 O 3−δ .…”
Section: Grain Boundary Conductivity In Nanoperovskitesmentioning
confidence: 91%
“…But some perovskites showed a decrease in conductivity due to the higher resistance shown by the grain boundaries. By incorporating a threshold amount of metals like platinum, it was observed that the electrical conductivity of protonic and oxide ionic conductors could be brought down significantly [120]. In certain cases, additional doping has also improved the conductivity [121][122][123][124][125].…”
Section: Grain Boundary Conductivity In Nanoperovskitesmentioning
confidence: 99%