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Mizusaki, Junichiro,Harita, Hideki,Mori, Naoya,Dokiya, Masayuki,Tagawa, Hiroaki The Korean Ceramic Society 2000 The Korean journal of ceramics Vol.6 No.2
At the porous $La_{0.6}Ca_{0.4}MnO_{3-{\delta}}$(LCM)/YSZ electrodes of solid oxide fuel cells (SOFC), the electrochemical redox reaction of oxygen proceeds via the triple boundary (TPB) of gas/LCM/YSZ. The surface diffusion of adsorbed oxygen on LCM has been proposed as the rate determining process, assuming the gradient of oxygen chemical potential from the outer surface of porous layer to TPB. Along with the formation of this gradient, oxygen nonstoichiometry in the bulk of LCM may varies. In this paper, an electrochemical technique was described precisely to determine the variation of oxygen content in LCM of porous LCM/YSZ under polarization. It was shown that the oxygen potential in LCM layer under large cathodic polarization is much lower than that in the gas phase, being determined from the electrode potential and Nernst equation.
T. Ohnishi,S. Mizusaki,M. Naito,Y. Nagata,M. Itou,Y. Sakurai,T. C. Ozawa,Y. Noro,H. Samata 한국물리학회 2013 THE JOURNAL OF THE KOREAN PHYSICAL SOCIETY Vol.62 No.12
The crystallographic, magnetic and transport properties of Sr1−xCaxRu0.5Mn0.5O3 were studiedto reveal the effects of crystal symmetry on the magnetism and the transport properties of antiferromagneticSrRu1−yMnyO3 (y > 0.2). The Ca-content dependences of the lattice constants and volumesuggest that the mixed valence state of Mn3+, Mn4+, Ru4+, and Ru5+ ions in SrRu0.5Mn0.5O3is held for Ca substitution. However, a structural transformation from tetragonal to orthorhombicsymmetry occurs at a Ca content of x 0.2, and a ferromagnetic state appears simultaneously. The Weiss temperature of all samples has a positive value regardless of the magnetic state. Theresistivity decreases as the Ca content increases, and the high temperature part of the resistivitycould be fitted by using the variable range hopping (VRH) model. The localization length increasesas soon as ferromagnetism appears. The Curie temperature seems to depend on the distance betweentransition metal ions. The antiferromagnetic state was explained by using the competitionbetween a ferromagnetic interaction along the c-axis and an antiferromagnetic interaction in theab-plane, and the orthorhombic ferromagnetic state was explained by using a three-dimensionalferromagnetic interaction between Mn ions.
Phonon echoes in Si:P at very low temperature
Jeong, M,Song, M,Ueno, T,Mizusaki, T,Matsubara, A,Lee, S Institute of Physics 2009 Journal of physics. Conference series Vol.150 No.4
<P>We observed phonon echoes in P-doped Si (Si:P) at very low temperatures. We applied two radio-frequency pulses separated by a time delay of τ on Si:P and observed echo signal at <I>t</I> &equal; 2τ in both insulating and metallic samples with varying dopant concentrations and of different sample forms of powders and bulk plates at temperature between 45 mK and 4 K. The echoes were much more pronounced in insulating powder samples than in metallic ones and in bulk ones. The echo intensity for a fixed τ increased very strongly as temperature was lowered but the echoes disappeared toward the superfluid-to-normal transition temperature of helium mixture in which the samples were immersed. We observed no appreciable change in the echo intensities as external magnetic field was varied up to 8 T. The echoes are interpreted to be dynamical polarization phonon echoes in piezoelectric powders of insulating Si:P with a dopant concentration <I>n</I> &equal; 6 x 10<SUP>17</SUP> cm<SUP>-3</SUP>.</P>
Kawamura, Ken-ichi,Watanabe, Kensuke,Nigara, Yutaka,Kaimai, Atsushi,Kawada, Tatsuya,Mizusaki, Junichiro The Korean Ceramic Society 1998 The Korean journal of ceramics Vol.4 No.2
The total conductivity and oxygen permeation in (Ce1-xZrxO2)0.9(CaO)0.1 solid solutions were measure das a function of temperature and oxygen partial pressure. Empirically, σ at given x and T was expressed essentially by σ=σo2+σeo Po2-1/4, where σo2 and σeo are constant. Applying a standard defect model in which major defects are Cace", Cece' and Vo in ideal solution, we can assign σo2 as the oxide ion conductivity decreases while the electronic conductivity increases with the increase in Zr content. Using the oxide ion and electronic conductivities thus determined, the oxygen permeation flux was calculated for respective Po2 and T conditions at which the measurements were made. The calculated values were found to agree with the observed ones.
Song, Myeonghun,Jeong, Minki,Kang, Byeongki,Lee, Soonchil,Ueno, Tomohiro,Matsubara, Akira,Mizusaki, Takao,Fujii, Yutaka,Mitsudo, Seitaro,Chiba, Meiro IOP Pub 2010 Journal of Physics, Condensed Matter Vol.22 No.20
<P>We present the spin dynamics of isolated donor electrons in phosphorus-doped silicon at low temperature and in a high magnetic field. We performed a steady-state electron spin resonance (ESR) on the sample with a dopant concentration of 6.5 × 10<SUP>16</SUP> cm<SUP> − 3</SUP> in a high field of 2.87 T (80 GHz) and at temperatures from 48 down to 1.8 K. As the temperature decreases below 16 K, the resonance spectral line changes from the usual derivative form characteristic of absorptions. Very long spin–lattice relaxation time <I>T</I><SUB>1</SUB> at low temperature gives rise to rapid passage effects and results in a dramatic change in the line shape and intensity as a function of temperature. We show that the numerical analysis based on the passage effects well explains the observed spectral changes with temperature. The spin–lattice relaxation time <I>T</I><SUB>1</SUB> is derived by numerical fit to the experimental data. We discuss the dynamic nuclear polarization of <SUP>31</SUP>P nuclear spins which shows up as asymmetric intensities of the hyperfine-split ESR resonance lines.</P>
Microscopic control ofSi29nuclear spins near phosphorus donors in silicon
Jä,rvinen, J.,Zvezdov, D.,Ahokas, J.,Sheludyakov, S.,Vainio, O.,Lehtonen, L.,Vasiliev, S.,Fujii, Y.,Mitsudo, S.,Mizusaki, T.,Gwak, M.,Lee, SangGap,Lee, Soonchil,Vlasenko, L. American Physical Society 2015 Physical review. B, Condensed matter and materials Vol.92 No.12