• Title/Summary/Keyword: $La_{0.2}Ca_{0.8}MnO_3$ CMR

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Characteristics of La0.2Ca0.8MnO3 Powder and Pellet Prepared by Sol-Gel Process (졸-겔법으로 합성한 La0.2Ca0.8MnO3의 분말과 펠렛의 특성)

  • Jung, Miewon;Lee, Jiyun;Kim, Hyunjung
    • Applied Chemistry for Engineering
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    • v.16 no.1
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    • pp.150-152
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    • 2005
  • $La_{0.2}Ca_{0.8}MnO_3$ colossal magnetoresistance (CMR) powders and pellets were synthesized by sol-gel process involving a stable metal chelate complex with acetylacetone. The structural changes of reaction mixture were monitored by FT-IR spectroscopy and X-ray diffractometry. The microstructure of sintered samples and the cation composition of gel powder were studied by FE-SEM/EDS and ICP-AES. The magnetic property was investigated as a function of temperature.

Magnetic and transport properties of $La_{0.8}Sr_{0.2}MnO_3/La_{0.8}Ca_{0.2}MnO_3$ bilayer

  • Li, S.F.;Kim, J.B.;Hyun, Y.H.;Lee, Y.P.;Prokhorov, V.G.;Komashko, V.A.
    • Journal of Korean Vacuum Science & Technology
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    • v.7 no.1
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    • pp.8-12
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    • 2003
  • The effects of lattice strain on the magnetic and the transport properties of La$_{0.8}$Sr$_{0.2}$MnO$_3$films grown on a LaAlO$_3$ (001) substrate and on a La$_{0.8}$Sr$_{0.2}$MnO$_3$ layer have been studied. It was observed that the metal-insulator and the ferromagnetic transitions turn out to be at higher temperatures for the film deposited on La$_{0.8}$Sr$_{0.2}$MnO$_3$ layer with respect to that on LaAlO$_3$. The dependence of Curie temperature on the bulk and the Jahn-Teller strains has also been determined. determined.

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Preparation and Characterization of La0.8Ca0.2MnO3 (La0.8Ca0.2MnO3의 합성 및 특성연구)

  • 정미원;이지윤;김현정
    • Journal of the Korean Ceramic Society
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    • v.40 no.5
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    • pp.434-440
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    • 2003
  • The powders of L $a_{0.8}$C $a_{0.2}$Mn $O_3$ Colossal Magnetoresistance (CMR) materials were synthesized by sol-gel process. Lanthanum(H), Calcium(II) and Manganese(III) 2,4-Pentanedionate were dissolved in a mixed binary solution consisted of propionic acid and methanol with PEG (15 wt%) aqueous solution. The progress of reactions was monitored by FT-IR spectroscopy. The Lao scao.2Mn03 gel powders were annealed at various temperatures. The structural changes were investigated by FT-IR, CP/MAS $^{ 13}$C solid state NMR spectroscopy and XRD. The thermochemical property, particle characterization, microstructure of sintered sample, and cation composition of gel powder were studied by TG/DTA, FE-SEM and ICP-AES. The magnetic characterizations were identified through measurement of magnetic moment by VSM.

$La_{0.7}Ca_{0.3-x}Ba_xMnO_3$ manganites : Local structure and transport properties

  • A.N.Ulyanov;Yang, Dong-Seok;Yu, Seong-Cho
    • Proceedings of the Korea Crystallographic Association Conference
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    • 2003.05a
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    • pp.8-8
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    • 2003
  • Electron-phonon interaction plays a significant role in forming of colossal magnetoresistance effect (CMR). Polaron formation was observed by neutron diffraction and by extended X-ray absorption fine structure (EXAFS) analysis. Local probe as given by the EXAFS is a useful method to study the polaronic charge and its dependence on temperature and ions size. Here we present the EXAFS study of polaronic charge in La/sub 0.7/Ca/sub 0.3-X/Ba/sub X/MnO₃ compositions. The single phase La/sub 0.7/Ca/sub 0.3-X/Ba/sub X/MnO₃ manganites (x=0; 0.03; 0.06, ..., 0.3) were prepared by ceramic technology [1]. The Curie temperature was determined by extrapolation of the temperature dependence of the magnetization (down to zero magnetization). EXAFS experiments were carried out at the 7C EC beam line of the Pohang Light Source (PLS) in Korea. The atomic pair distribution functions (PDF) were obtained by re-regularization method [2] from filtered spectra. The PDF for the x=0.3 sample showed a single peak function and for x=0.0, 0.03, 0.06, 0.09, 0.12 compositions were asymmetric in agreement with a small Jahn-Teller elongation of two (short and long) bonds of the MnO/sub 6/ octahedron. Dispersion, σ/sub Min-O//sup 2/, and asymmetry, σ/sub Min-O//sup 3/, of the Mn-O bond distances varied significantly with x and showed a maximums at x=0.09. The maximum of σ/sub Min-O//sup 2/ is caused by increase of dynamic rms displacements of the Mn-O distances near the T/sub C/. The observed x dependence of σ/sub Min-O//sup 3/ reflects the reduction of charge carriers mobility at approaching to T/sub C/ from low as well as high temperatures.

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