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000014013 0247_ $$2DOI$$a10.1111/j.1551-2916.2010.04011.x
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000014013 041__ $$aENG
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000014013 084__ $$2WoS$$aMaterials Science, Ceramics
000014013 1001_ $$0P:(DE-Juel1)VDB88648$$aYoon, S.$$b0$$uFZJ
000014013 245__ $$aElectronic conduction mechanisms in BaTiO3-Ni composites with ultrafine microstructure
000014013 260__ $$aOxford [u.a.]$$bWiley-Blackwell$$c2010
000014013 300__ $$a4075 - 4080
000014013 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
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000014013 440_0 $$03845$$aJournal of the American Ceramic Society$$v93$$x0002-7820$$y12
000014013 500__ $$aThis work was financially supported by a Korea Research Foundation Grant funded by the Korean Government (KRF-2007-D00124).The authors are grateful to Dr. Heinz-Josef Penkalla for support by electron microscopy and spectroscopy and to Dr. Detlev Hennings for the helpful discussion and comments. S. Yoon acknowledges the support from COST Action 539 (COST-STSM-539-03589) of the European Union. NAMICS Corporation, Niigata (Japan) is gratefully acknowledged for financial support within a common collaboration project.
000014013 520__ $$aSpark plasma sintering (SPS) was used to densify BaTiO3–Ni composite powders to relative densities above 92.8%. With the increasing Ni content, a decrease in relative density is observed, suggesting that Ni hampers the consolidation process. The microstructures of the BaTiO3–Ni composites were of duplex character. The crystallite size of the BaTiO3-grains was around 100 nm in average. The ceramic matrix phase of BaTiO3 surrounded Ni inclusions of approximately 1 μm in diameter that were completely incorporated without the formation of any elongated metallic filaments. The ac conductivity of these BaTiO3–Ni composites increased with increasing Ni content and with temperature. The dominant conduction mechanisms in SPSed BaTiO3–Ni composites showed quite a complicated behavior. A gradual change from band conduction of trapped electrons in oxygen vacancies to a hopping-type motion of small polarons between Ti4+ and Ti3+ is suggested to occur, when the Ni content increases. The influence of oxygen vacancies and other lattice defects on the electrical properties of BaTiO3–Ni composites is discussed.
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000014013 7001_ $$0P:(DE-Juel1)130894$$aPithan, C.$$b1$$uFZJ
000014013 7001_ $$0P:(DE-Juel1)131022$$aWaser, R.$$b2$$uFZJ
000014013 7001_ $$0P:(DE-Juel1)129189$$aDornseiffer, J.$$b3$$uFZJ
000014013 7001_ $$0P:(DE-HGF)0$$aXiong, Y.$$b4
000014013 7001_ $$0P:(DE-HGF)0$$aGruner, D.$$b5
000014013 7001_ $$0P:(DE-HGF)0$$aShen, Z.$$b6
000014013 7001_ $$0P:(DE-HGF)0$$aIwaya, S.$$b7
000014013 773__ $$0PERI:(DE-600)2008170-4$$a10.1111/j.1551-2916.2010.04011.x$$gVol. 93, p. 4075 - 4080$$p4075 - 4080$$q93<4075 - 4080$$tJournal of the American Ceramic Society$$v93$$x0002-7820$$y2010
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