• 한국세라믹학회지
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• 제28권8호
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• pp.603-610
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• 1991

An oxygen deficient perovskite (CaLa)(MgMn)O5.43, with the cubic unit cell parameter of 3.826$\AA$, was prepared 115$0^{\circ}C$ for 10 hrs under the ambient oxygen gas pressure. The average oxidation state of manganese was determined to be 3.86 by the iodometric titration, so that the perovskite could be formulated as (CaLa) ({{{{ { MgMn}`_{ chi } ^{II } }}{{{{ { Mn}`_{ y} ^{III } }}{{{{ { Mn}`_{1- chi -y } ^{IV } }})O5.43 (2x+y=0.14). From X-ray photoelectron spectroscopy, the manganese ions in the lattice are mostly tetravalent, but two paramagnetic configurations were observed in the EPR spectrum: One sharp isotropic signal with hyperfines (ΔH 50 G, g=1.997$\pm$0.002 and │A│=82(4)$\times$10-4 cm-1) and a broad isotropic one (ΔH 1600 G, g=1.994$\pm$0.002), those which correspond respectively to Mn(II) and Mn(IV) ions. According to the magnetic susceptibility measurement, it follows the Curie-Weiss law from 20 K up to room temperature with $\mu$eff=5.23 $\mu$B, which is relatively larger than spin-only value({{{{ { mu }`_{eff} ^{s.o } }}=4.04 $\mu$B) due to the effect of weak ferromagnetic coupling. Such a result is in accord with a theory of semicovalence exchange.

• 한국자기학회지
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• 제5권5호
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• pp.432-436
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• 1995

The hydrogen decrepitation behaviour of the $Sm_{2}Fe_{17} alloy containing 4at%Nb was examined by means of DTA and SEM metallography, and the magnetic properties of the alloy were studied by means of VSM or TMA. It has been found that a simple hydrogenation and degassing treatment for the alloy caused a poor hydrogen decrepitation. The cycle treatment consisting of repeated hydrogenation and degassing, however, caused a severe hydrogen decrepitation with a combination of intergranular and transgranular failure. The disproportionation temperature of the hydrogenated $Sm_{2}Fe_{17}-type alloy was enhanced significantly by small addition of Nb. It has also been found that the Curie temperature of $Sm_{2}Fe_{17} matrix phase in the Nb-containing alloy has been enhanced by the hydrogenation, and this was attributed to the increase in interatomic distance between the neighbouring iron atoms caused by the interstitial occupancy of the hydrogen atom into the $Sm_{2}Fe_{17}-type lattice. The magnetisation of the $Sm_{2}Fe_{17} alloy containing Nbwas found to be lower than that of the Nb-free alloy, and this was explained by the dilution effect due to the presence of the paramagnetic $Sm_{2}Fe_{17} phase.

• Journal of Magnetics
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• 제10권3호
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• pp.95-98
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• 2005

We report hole-induced ferromagnetism in diluted magnetic semiconductor $Zn_{0.99}Mn_{0.01}$ films grown on $SiO_2/Si$ substrates by reactive sputtering. The p-type conduction with hole concentration over $10^{18}\;cm^{-3}$ is achieved by P doping followed by rapid thermal annealing at $800^{\circ}C$ in a $N_2$ atmosphere. The p-type $Zn_{0.99}Mn_{0.01}O:P$ is carefully examined by x-ray diffraction and transmission electron microscopy. The magnetic measurements for $p-Zn_{0.99}Mn_{0.01}O:P$ clearly reveal ferromagnetic characteristics with a Curie temperature above room temperature, whereas those for $n-Zn_{0.99}Mn_{0.01}O:P$ show paramagnetic behavior. The anomalous Hall effect at room temperature is observed for the p-type film. This result strongly supports hole-induced room temperature ferromagnetism in $p-Zn_{0.99}Mn_{0.01}O:P$.

• 한국재료학회지
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• 제28권8호
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• pp.445-451
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• 2018

We report the structural, magnetic and magnetocaloric properties of $Sr_{1.8}Pr_{0.2}FeMo_{1-x}W_xO_6$($0.0{\leq}x{\leq}0.4$) samples prepared by the conventional solid state reaction method. The X-ray diffraction analysis confirms the formation of the tetragonal double perovskite structure with a I4/mmm space group in all the synthesized samples. The temperature dependent magnetization measurements reveal that all the samples go through a ferromagnetic to paramagnetic phase transition with an increasing temperature. The Arrott plot obtained for each synthesized sample demonstrates the second order nature of the magnetic phase transition. A magnetic entropy change is obtained from the magnetic isotherms. The values of maximum magnetic entropy change and relative cooling power at an applied field of 2.5 T are found to be $0.40Jkg^{-1}K^{-1}$ and $69Jkg^{-1}$ respectively for the $Sr_{1.8}Pr_{0.2}FeMoO_6$ sample. The tunability of magnetization and excellent magnetocaloric features at low applied magnetic field make these materials attractive for use in magnetic refrigeration technology.

• 한국자기학회지
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• 제20권6호
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• pp.216-221
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• 2010

본 연구에서는 dimethylacetamide(DMAc)와 toluen을 용매로 사용하여 만들어진 양친매성 urethan acrylate nonionomer(UAN) 선구고리를 기초로 하는 양친매성 고분자 망상구조 복합체에 철산화물을 주입시킨 나노복합체의 구조와 자기적성질 그리고 나노복합체에 존재하는 Fe 이온의 원자가 상태를 알아보기 위하여 전계방출주사전자현미경(FESEM)과 X-ray diffraction 그리고 Mossbauer spectrum을 측정하였다. 결과로부터 나노복합체 시료 내에 존재하는 모든 Fe이온은 $Fe^{3+}$의 상태로 존재하고 $Fe_2O_3$의 결정구조를 갖고 있음을 알 수 있으며, 시료 내에 철산화물 나노복합체가 형성되어 있음을 알 수 있었다. 그리고 urethan acrylate nonionomer(UAN) 선구 고리를 기초로 하는 양친매성 고분자 망상구조 복합체를 형성시키는 경우 용매로 DMAc를 이용하는 경우가 toluen을 이용한 경우 보다 더 미세한 나노구조를 형성함을 알 수 있으며, 시료들의 자기적 성질이 상온에서 상자성을 나타내는 것은 나노크기의 단일자구형성에 따른 초상자성효과에 의한 것임을 알 수 있었다.

• 한국자기학회지
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• 제8권4호
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• pp.192-197
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• 1998

Ni1-xCdxFeAlO4계의 Mossbauer 스펙트럼은 x가 0.2이하인 경우에는 초상자성 이완 현상을, x가 0.3∼0.5인 경우는 준강자성에 의한 sextet를, x가 0.7, 0.8인 경우에는 강자성 이완 현상, x가 0.8이상인 경우에는 상자성에 dmlgksdoublet가 나타난다. x가 0.2이하인 시료에서 치환된 Cd2+이온은 주로 A-site의 Fe3+이온도 B-site로 이동하게 된다. Ni1-xCdxFeAlO4계의 초상자성 이완 현상은 A-site의 A13+이온에 의한 것으로, 강자성 이완현상은 치환된 Cd2+이온에 의한 것으로 설명할 수 있고, Yafet-Kittel 자기구조에 따라 Ni1-xCdxFeAlO4계의 자기적 성질을 해석할 수 있다.

• 한국광물학회지
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• 제27권4호
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• pp.311-320
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• 2014

슬래그를 매립한 토양을 대상으로 자기분리연구를 수행하였다. 토양세척을 거친 토양과 토양세척 전 토양을 대상으로 습식자기분리와 건식자기분리를 수행하여 분리된 부분과 분리되지 않은 부분의 중금속 농도를 측정하여 중금속의 농축효과를 측정하였다. 습식자기분리의 경우 토양세척 전 시료의 자력분리율이 상대적으로 높으며 토양세척 후 시료의 경우 약 40% 정도가 자기분리 되었다. 토양 : 물의 비가 농축효과에는 큰 영향을 미치지 못하며, Fe, Pb, Cu, Zn, Cd의 세척 전 토양과 세척 후 토양의 자기분리에 의한 평균 농축비는 3.2, 2.1, 12.1, 2.5, 1.5와 17.4, 7.0, 15.7, 9.6, 7.0으로 토양 세척을 거친 경우 자기분리에 의해 토양 세척 전 토양에 비해 더 큰 토양 부피 감량효과를 기대할 수 있다. 건식자기분리의 경우에도 자기분리에 의해 중금속의 농축효과를 얻을 수 있으나 자기분리에 의한 회수율이 너무 높은 경우 오염토 저감을 기대하기 어렵다. 철과 같은 강자성체를 포함하는 토양의 경우 자기분리에 의해 토양세척의 효과와 유사하게 오염토양의 양을 줄일 수 있고, 오염이 한쪽에 농축되는 결과를 얻을 수 있다.

• 한국광물학회지
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• 제10권2호
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• pp.148-161
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• 1997

Based on the X-ray powder diffraction (XRD) and M ssbauer spectroscopy, the thermal behavior and phase transformations of two clays are investigated for raw and fired conditions, which are collected from Kwangryeongli and Ildo district in Cheju Island. M ssbauer spectra at room temperature and 20for two clays show that paramagnetic Fe3- is the structural iron of the layer silicate and ferrihydrite, and superparamagnetic goethite has about 50% of total iron contents. The XRD peaks of hematite for the fired clays appear from 80$0^{\circ}C$ in Kwangryeongli clay and from $600^{\circ}C$ in Ildo district clay, respectively. The structural Fe2+ was completely oxidized into Fe3- at 40$0^{\circ}C$ for Kwangryeongli clay and 50$0^{\circ}C$~$600^{\circ}C$ for Ildo district clay, respectively. The structural Fe2+ was completely oxidized into Fe3- at 40$0^{\circ}C$. For the temperature ranging from 40$0^{\circ}C$ to $700^{\circ}C$~80$0^{\circ}C$, two fired clays exhibit the dehydroxylation of the clay mineral. A disintegration of the clay mineral structure is observed from $700^{\circ}C$~80$0^{\circ}C$ to 110$0^{\circ}C$, followed by the onset and spread of vitrification process. It is also shown that well-crystallized hematite phase is formed at the temperature higher than 110$0^{\circ}C$ and the relative absorption area decreases, which might be related to the recrystallization of alluminosilicate matrix.

• 한국분말재료학회지
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• 제13권4호
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• pp.285-289
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• 2006

Co-Fe-Ni-B-Si-Cr based amorphous strips containing nitrogen were manufactured via melt spinning, and then devitrified by crystallization treatment at the various annealing temperatures of $300^{\circ}C{\sim}540^{\circ}C$ for up to 30 minutes in an inert gas $(N_2)$ atmosphere. The microstructures were examined by using XRD and TEM and the magnetic properties were measured by using VSM and B-H meter. Among the alloys, the amorphous ribbons of $Co_{72.6}Fe_{9.8}Ni_{5.5}B_{2.4}Si_{7.1}Cr_{2.6}$ containing 121 ppm of nitrogen showed relatively high saturation magnetization. The alloy ribbons crystallized at $540^{\circ}C$ showed that the grain size of $Co_{72.6}Fe_{9.8}Ni_{5.5}B_{2.4}Si_{7.1}Cr_{2.6}$ alloy containing 121 ppm of nitrogen was about f nm, which exhibited paramagnetic behavior. The formation of nano-grain structure was attributed to the finely dispersed Fe4N particles and the solid-solutionized nitrogen atoms in the matrix. Accordingly, it can be concluded that the nano-grain structure of 5nm in size could reduce the core loss within the normally applied magnetic field of 300A/m at 10kHz.

• 한국초전도학회:학술대회논문집
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• 한국초전도학회 1999년도 High Temperature Superconductivity Vol.IX
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• pp.210-213
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• 1999

Magnetoresistance and magnetization of Sr$_{l-x}K_xBiO_3$ were both measured as functions of temperature and magnetic field. Resistivity goes to zero at T=10.1K and the overall superconducting transition behavior under applied magnetic fields is similar to that of other BiO based superconductors. Also, below T<5K we have observed the reappearance of finite resistivity with a power law temperature dependence( ${\rho}$ ${\sim}$T$^1$); the reentrant superconducting transition of resistivity. Contrary to the Josephson weak link effect in polycrystalline samples, which gives the depression of the superconducting state with increasing electrical current or magnetic field, the superconducting state for T<5K is resumed by applying a higher current or magnetic field. Magnetic susceptibility( ${\chi}$ ) of Sr$_{l-x}K_xBiO_3$ for T<5K also shows similar trends to that observed in transport measurements: increase of ${\chi}$ (paramagnetic-like behavior) at a low magnetic fields(B=50 Oe) and, the resumption of perfect diamagnetism at high fields.