• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.151.1-151.1
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• 2016

Complex oxide heterointerfaces have been extensively explored in the past due to the novel phenomenon emerging at such interfaces that differ from their individual bulk counterparts. The integration of a ferromagnetic (FM) material with the superconducting (SC) material leading to proximity effect is one of the commonly studied phenomenon in these heterostructures. In continuation, we have stabilized the FM layer La0.7Ca0.3MnO3 (LCMO) on SC material YBa2Cu3O7-${\delta}$ (YBCO) using pulsed laser deposition technique and explored the structural, magnetic, electrical and magneto-transport properties of this heterostructure. ${\Phi}$-scan measurements confirm the epitaxial nature of LCMO/YBCO heterostructure grown on single crystalline SrTiO3 substrate. The FM transition of LCMO and SC transition of YBCO are observed in the magnetization measurements of the bilayer structure. Through electrical measurements, we understood that the proximity effect leads to lowering of the SC transition of YBCO. The role of interface in the bilayer structure is also realized through electrical transport measurements.

• Proceedings of the Korean Magnestics Society Conference
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• 1996.05a
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• pp.32-33
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• 1996

• Proceedings of the Korean Vacuum Society Conference
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• 1999.07a
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• pp.145-145
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• 1999

La-Ca-Mn-O (LCMO) 박막에서 초거대 자기 저항 효과와 발견된 이후 자기 센서와 고밀도 자기 저장 매체로서 응용하기 위한 연구가 진행되고 있다. 그러나 현재 대부분의 증착은 타겟과 박막간의 조성의 일치를 위하여 PLD 방법을 이용하고 있으며 RF magnetron sputtering 법으로 증착한 예는 많이 보고되고 있지 않으며 특히 적층 성장시킨 예는 아직 보고되지 있지 않다. 또한 LCMO와의 낮은 격자 상수 불일치를 보이는 SrTiO3와 LaAlO3 기판에 LCMO 박막을 성장시킬 경우 LaAlO3의 경우 XRD rocking curve의 curve의 FWHM 값이 SrTiO3 상에 증착시킨 것의 10배 이상의 값을 보인다는 것은 주목할 만한 사실이다. RF magnetron sputtering 법을 이용하여 LaAlO3 기판상에 145nm MCMO 박막을 적층성장시켰다. XRD $ heta$-2$\theta$ scan을 통해 박막이 c-축 배향한 것을 확인할 수 있었으며 RBS 분석결과 4.98%의 minimumyield를 보였으며 이로부터 박막이 적층성장한 것을 확인할 수 있었다. LCMO (200) peak의 XRD $\theta$-rocking 결과 FWHM의 값은 0.311$^{\circ}$를 보였으나 2개의 피크가 존재하는 것을 볼 수 있었다. 따라서 기판의 (200) 피크를 XRD $\theta$-2$\theta$ scan에서 0.3$^{\circ}$ 간격으로 두 개의 피크를 관찰할 수 있었는데 이는 기판과 박막간의 stress로 인한 tetragonal distortion에 의한 것으로 알려져 있었다. 따라서 기판상에 박막이 어떤 식으로 적층 성장되었는지를 RBS를 이용하여 <001>과 <011> 방향으로 2MeV He++를 주입하여 0.1$^{\circ}$ 간격으로 틸팅을 해본 결과 <001> 방향에서는 1.12$^{\circ}$의 차이를 보였다. 이는 기판과의 compressive stress로 인해 c축 방향으로 늘어났으며 stress relaxed layer는 XRD 결과와는 달리 관찰할 수 없었다. 이러한 현상의 기판 자체의 twin 구조로 인한 것으로 생각된다. RBS 분석후 고분해능 XRD를 이용해 LCMO (200) peak의 $\theta$-rocking 결과 이제R지 laAlO3 상 증착한 LCMO의 값으로는 제일 작은 0.147$^{\circ}$를 나타내었다.

• Journal of the Korean Electrochemical Society
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• v.20 no.3
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• pp.55-59
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• 2017

In this study, thermoelectric characteristics of perovskite $La_{0.5}Ca_{0.5}MnO_3$ (LCMO) nanomaterials were investigated by theoretical simulation and experimental analysis. Thermoelectric power factors calculated by DFT simulation were gradually enhanced as increase in annealing temperature. Maximum power factor was obtained with high magnitude of $S^2{\sigma}=566{\mu}W/m{\cdot}K^2$ at 1100 K through a dominant improvement of Seebeck coefficient compared with electrical conductivity. Experimentally, the LCMO nanomaterials were hydrothermally synthesized and then treated by post thermal annealing with temperature variation. X-ray diffraction and SEM analysis illustrated that LCMO exhibited orthorhombic perovskite structures with small grain size of 16~19 nm over 873 K. The results directly confirmed that improvement of crystallinity and decrease of mean grain size given by post thermal annealing lead to enhancements of electrical conductivity and Seebeck coefficient, respectively.

• Proceedings of the Korean Magnestics Society Conference
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• 1997.05a
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• pp.110-111
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• 1997

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.9 no.4
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• pp.384-386
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• 1999

The distribution coefficients of Ni and Zn to the Cu site in $La_{2-x}Sr_{x}CuO_{4}$(LCO) were investigated to determine the suitable solvent composition ofr crystal growth of $La_{2}{Cu}_{1-x}{M}_{x}{O}_{4}$(M=NI, Zn)(LCMO), and were found to be 4.2 for NI and 0.66 for Zn, respectively. Single crystals of LCO, and LCMO of high homogeneity were grown by traveling solvent floating zone technique using suitable solvents. NO diamagnetic signals were observed for all substituted crystals. This fact suggests that crystals of LCO partially substituted by Ni or Zn are useful as substrate crystals.

• Proceedings of the Korean Magnestics Society Conference
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• 2008.12a
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• pp.159.1-159.1
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• 2008

• Bulletin of the Korean Chemical Society
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• v.25 no.2
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• pp.182-184
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• 2004

Fine $La_{2/3}Ca_{1/3}MnO_3$ nanocrystalline powders have been successfully prepared by modified citrate pyrolysis process. The obtained LCMO nanoscale grains have a mean particle size of about 30 nm under optimal treatment conditions. The particle size can be controlled by adjusting processing parameters, such as treatment temperature and calcination time. X-ray diffraction, SEM and magnetoresistance effect were employed to study the crystal structure, morphology and magnetic property of these nanosized powders. A novel MR effect (MR > 45% (0 K < T < 340 K)) at room temperature has been found.

• Journal of the Korean Magnetics Society
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• v.8 no.4
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• pp.179-184
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• 1998

Colossal magnetoresistance is closely related to (but is not) the abrupt change of electrical resistivity in the vicinity of Curie temperature, which is caused by the temperature dependent paramagnetic-ferromagnetic phase transition and concurrent change of electrical conducting mechanism. A resistivity-temperature equation is presented to fully describe the overall behavior, especially the abrupt change. The main ingredients of the equation are a simple effective media theory and a function for the temperature dependent fraction of ferromagnetic phase. The model fits very well to the measured resistivity-temperature curve of $La_{0.7}Ca_{0.3}MnO_3$.

• Korean Journal of Materials Research
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• v.21 no.4
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• pp.216-219
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• 2011

Perovskite manganites such as $RE_{1-x}A_xMnO_3$ (RE = rare earth, A = Ca, Sr, Ba) have been the subject of intense research in the last few years, ever since the discovery that these systems demonstrate colossal magnetoresistance (CMR). The CMR is usually explained with the double-exchange (DE) mechanism, and CMR materials have potential applications for magnetic switching, recording devices, and more. However, the intrinsic CMR effect is usually found under the conditions of a magnetic field of several Teslas and a narrow temperature range near the Curie temperature ($T_c$). This magnetic field and temperature range make practical applications impossible. Recently, another type of MR, called the low-field magnetoresistance(LFMR), has also been a research focus. This MR is typically found in polycrystalline half-metallic ferromagnets, and is associated with the spin-dependent charge transport across grain boundaries. Composites with compositions $La_{0.7}(Ca_{1-x}Sr_x)_{0.3}MnO_3)]_{0.99}/(BaTiO_3)_{0.01}$ $[(LCSMO)_{0.99}/(BTO)_{0.01}]$were prepared with different Sr doping levels x by a standard ceramic technique, and their electrical transport and magnetoresistance (MR) properties were investigated. The structure and morphology of the composites were studied by X-ray diffraction (XRD) and scanning electronic microscopy (SEM). BTO peaks could not be found in the XRD pattern because the amount of BTO in the composites was too small. As the content of x decreased, the crystal structure changed from orthorhombic to rhombohedral. This change can be explained by the fact that the crystal structure of pure LCMO is orthorhombic and the crystal structure of pure LSMO is rhombohedral. The SEM results indicate that LCSMO and BTO coexist in the composites and BTO mostly segregates at the grain boundaries of LCSMO, which are in accordance with the results of the magnetic measurements. The resistivity of all the composites was measured in the range of 90-400K at 0T, 0.5T magnetic field. The result indicates that the MR of the composites increases systematically as the Ca concentration increases, although the transition temperature $T_c$ shifts to a lower range.