• 공업화학
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• 제16권1호
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• pp.150-152
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• 2005

아세틸아세톤이 치환된 금속-킬레이트 착물에 polyethylene glycol를 첨가시켜 안정하고 균일한 졸 용액을 얻은 뒤, 페로보스카이트 $La_{0.2}Ca_{0.8}MnO_3$의 분말과 펠렛을 합성하였다. 반응과정에 대한 구조변화를 FT-IR과 XRD 분석기로 추적하였고, 입자 크기와 균일도를 살펴보았다. 그리고 온도의 함수로서의 자기적 특성도 관찰하였다.

• Journal of Korean Vacuum Science & Technology
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• 제7권1호
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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.

• 한국세라믹학회지
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• 제40권5호
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• pp.434-440
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• 2003

초거대 자기 저항 물질인 페로브스카이트 L $a_{0.8}$C $a_{0.2}$Mn $O_3$의 분말을 졸-겔방법으로 제조하였다. Lanthanum(III), Calcium(II) 그리고 Manganese(III) 2,4-Pentanedionate를 Propionic acid와 methane떠 혼합용매를 사용하고 PEG (l5 wt%) 용액을 첨가 하여 안정한 졸용액을 합성하였고 FT-IR spectroscopy로 반응의 진행 정도를 관찰하였다. L $a_{0.8}$C $a_{0.2}$Mn $O_3$ 겔 분말에 대해 온도를 변화시키면서 열처리하여 FT-IR, CP/MAS $^{13}$C solid state NMR spectroscopy와 XRD등을 이용해 구조변화를 관찰하였다. 열분석은 TG/DTA로 측정하였으며, FE-SEM을 통해 입자크기와 균일도를 관찰하였고, 양이온 조성 비율을 알아보기 위해 ICP-AES를 측정하였다. 자성 특성을 규명하기 위해 VSM을 이용하여 자기 모멘트를 측정하였으며, 상자기성 에서 강자기성으로 전이되는 큐리온도( $T_{c}$)를 관찰하였다.

• 한국결정학회:학술대회논문집
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• 한국결정학회 2003년도 춘계학술연구발표회
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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.