• 대한화학회지
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• 제56권5호
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• pp.609-616
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• 2012

Ba-ferrite ($BaFe_{12}O_{19}$) nanoparticles were synthesized by chemical coprecipitation method in an aqueous solution. The particle size and the crystallization temperature of the Ba-ferrite nanoparticles were controlled varying the precipitation temperature. The precipitate that was prepared at $0^{\circ}C$ showed the crystal structure of Ba-ferrite in X-ray diffraction when it was calcined at the temperature above $580^{\circ}C$, whereas what was prepared at $50^{\circ}C$ showed the crystallinity when it was calcined at the temperature higher than about $700^{\circ}C$. The particle sizes of the synthesized Ba-ferrite were in a range of about 20-30 nm when it was prepared by being precipitated at $0^{\circ}C$ and calcined at $650^{\circ}C$. When the precipitation temperature increased, the particle size also increased even at the same calcination temperature. The magnetic properties of the Ba-ferrite nanoparticles were also controlled by the synthetic condition of precipitation and calcination temperature. The coercive force could be appreciably lowered without a loss of saturation magnetization when the Ba-ferrite nanoparticles were prepared by precipitation and calcination both at low temperatures.

• Journal of Magnetics
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• 제9권2호
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• pp.27-33
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• 2004

Magnetic properties of $Nd_4Fe_{77.5}B_{18.5}$ compound in term of exchange coupling between $Nd_2Fe_{14}B$ and $Fe_3B$ magnetic nano crystals in melt spun powders were characterized by varying the quenching speed in mass production line. The exchange coupled phenomenon was characterized as functions of nano crystal size and volume fraction of each magnetic phase which was possible by employing Henkel plot (${\delta}M$) and refined Mossbauer spectroscopy. The optimized magnetic properties obtained from the present volume production line were: $B_r= 11.73 kG,{_i}H_c/ = 3.082 kOe$, and $(BH)_{max} = 12.28 MGOe.$ The volume fraction of each magnetic phase for those conditions giving the grain size of 10 nm were ${\alpha}-Fe; 4.2%, Fe_3B; 60.1 %$, and $Nd_2Fe_{14}B; 35.7%$. The superior magnetic properties in the $Nd_2Fe_{14}Fe_3B$ based nanocomposites were confirmed to be dependant on the volume fraction of $Fe_3B$.

• 한국재료학회지
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• 제15권6호
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• pp.393-398
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• 2005

The crystal structure and magnetic properties of the $Mg_{1-x}Zn_xFeAlO_4\;(0{\leq}x\leq1.0)$ have been investigated by means of x-ray diffractometry and $M\ddot{o}ssbauer$ spectroscopy. The samples$(0{\leq}x\leq1.0)$ have been prepared by the ceramic sintering method. The x-ray diffraction pattern shows that the crystal structure of the samples is a cubic spinel type. The lattice constant has been found by extrapolation using the Nelson-Riley function and it increases slightly from $8.3496\AA\;to\;8.4128\AA$ with Zn concentration. The $M\ddot{o}ssbauer$ spectra for x<0.4 show a superposition of two sextets ana a paramagnetic doublet at room temperature. The superparamagnetic doublet for x<0.4 seems to be due to Al ion in tetrahedral site by the superparamagnetic clustering effect.

• Journal of Magnetics
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• 제7권2호
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• pp.40-44
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• 2002

Crystallographic and magnetic properties of ;$LaFe_{1-x}Ga_xO_3$($\chi$= 0, 0.1, 0.3, 0.5, and 0.7) were studied using XRD and Mossbauer spectroscopy. The crystal structures were found to be orthorhombic and the lattice parameters $\alpha$, b, and c were found to decrease with increasing Ga substitution. M$\ddot{o}$ssbauer spectra were obtained at various absorber temperatures ranging from 20 K to 750 K. The M$\ddot{o}$ssbauer spectra were all sextets below $T_N$ and were all singlets above $T_N$. Asymmetric broadening of the M$\ddot{o}$ssbauer spectral lines at 20 K was explained by the multitude of possible environments for an iron nucleus. As the temperature increases to $T_N$, a systematic line broadening in M$\ddot{o}$ssbauer spectra was observed and interpreted to originate from different temperature dependencies of the magnetic hyperfine fields at various iron sites.

• Bulletin of the Korean Chemical Society
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• 제15권7호
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• pp.541-545
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• 1994

A series of samples of the ${Ca_xEu_{1-x}FeO_{3-y}$ (x=0.00, 0.25, 0.50, 0.75, and 1.00) system has been prepared at $1,250^{\circ}C$ under an atmospheric air pressure. X-ray diffraction analysis of the solid solution assigns the structure of the compositions of x=0.00, 0.25, 0.50, and 0.75 to the orthoferrite-type orthorhombic system, and that of x=1.00 to the brownmillerite-type orthorhombic one. The mole ratios of $Fe^{4+}$ ion in the solid solutions or ${\tau}$ values were determined by the Mohr's salt analysis and nonstoichiometric chemical formulas of the system were formulated from x, ${\tau}$, and y values. From the result of the Mossbauer spectroscopy, the coordination and magnetic property of the iron ion are discussed. The electrical conductivities are measured as a function of temperature. The activation energy is minimum at the composition of x=0.25. The conduction mechanism can be explained by the hopping of electrons between the mixed valences of $Fe^{3+}\;and\;Fe^{4+}$ ions.

• Bulletin of the Korean Chemical Society
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• 제15권8호
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• pp.636-640
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• 1994

The nonstoichiometric perovskite solid solutions of the $Nd_{1-x}Sr_xFeO_{3-y}$ system for the compositions of x=0.00, 0.25, 0.50, 0.75, and 1.00 have been prepared at $1150^{\circ}C$ in the air pressure. The compound of x=0.00, NdFe$O_{3.0}$, contains only $Fe^{3+}$ ion in octahedral site and the others involves the mixed valence state between $Fe^{3+}$ and $Fe^{4+}$ ions. The mole ratio of $Fe^{4+}$ ion or the ${\tau}$-value increases steadily with the x-value and then is maximized at the compositionof x= 1.00. The nonstoichiometric chemical formulas of the system are formulated from the x, ${\tau}$ and y values. From the Mossbauer spectroscopy, the isomer shift of $Fe^{3+}$ ion decreases with the increasing x-value, which is induced by the electron transfer between the$Fe^{3+}$ and $Fe^{4+}$ ions. The transfer is made possible by the indirect interaction between $Fe^{3+}$ and$Fe^{4+}$ ions via the oxygen ion. The eg electrons of the$Fe^{3+}$ ions are delocalized over all the Fe ions. Due to the electron transfer, the activation energy of electrical conductivity is decrease with the increasing amount of $Fe^{4+}$ ion.

• 한국자기학회지
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• 제11권1호
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• pp.21-25
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• 2001

Si 기판 위에 $\alpha$-Fe$_2$O$_3$ 박막을 pulsed laser deposition system으로 제조하여 결정학적 및 자기적 성질을 X선 회절 및 Mossbauer 분광법을 사용하여 연구하였다. 박막의 제조조건은 laser의 출력 5.128 W/$cm^2$, 산소의 압력 0.1 torr, 기판의 온도 30$0^{\circ}C$에서 가장 이상적이었으며 이를 공기 중 80$0^{\circ}C$에서 1일간 열처리하였다. 입자는 크기는 길이 200~300nm, 폭 70-150 nm정도의 타원체로 기판에 비스듬히 누운 형태를 취하고 있으며 결정은 육방정계 형태의 corundum 구조로서 결정상수는 a = 5.03 0.05 $\AA$, c = 13.73$\pm$0.05 $\AA$로 측정되었다. 원자의 스핀 방향은 감마선 방향(기판에 수직 방향)에 대하여 평균적으로 Morin 변환 이하에서는 38$^{\circ}$, 그 이상에서는 48$^{\circ}$의 각을 이루며 특정한 방향을 선호하고있는 것으로 나타났다. Morin 변환은 200 K에서 실온가지 넓은 온도 범위에서 일어나며, c-축에 대한 원자의 스핀 방향은 48$^{\circ}$에서 80$^{\circ}$정도의 변화만이 관측되었다.

• 한국자기학회지
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• 제15권2호
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• pp.113-117
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• 2005

4-point focused floating Bone furnace를 이용하여 multiferroic $HoMnO_3$ 단결정을 제조하였으며, 직접합성법으로 $HoMn_{1-x}\;^57Fe_xO_3$ (x=0, 0.01, 0.02, 0.05) 분말 시료를 제조하여 그 결정학적 및 자기적 성질을 연구하였다. 결정구조는 hexagonal 구조로, (110) 방향이 자화용이축 임을 알 수 있었고, 온도 변화에 따른 강유전 상수(dielectric constant $\epsilon$)는 c축과 평행한 방향에서 특이성(anomaly)을 갖는 것으로 나타났다. 이 때 특이성이 나타나는 온도 구간은, c축 방향으로 인가된 자기장 세기에 따라 민감하게 변화함이 관측되고 있어, multiferroic 소자로의 응용 가능성을 제시하고 있다. 한편 Mn 자리에 $^{57}Fe$를 미량 치환한 분말 시료에 대하여 $M\ddot{o}ssbauer$ 분광학적 연구를 수행하였다.

• 한국자기학회지
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• 제15권2호
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• pp.137-141
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• 2005

Spinel계 유화물 $Zn_xFe_{1-x}Cr_2S_4$(x=0.05, 0.1, 0.2)에 대하여 X선 회절법, 자기저항측정, $M\ddot{o}ssbauer$ 분광법을 이용하여 CMR 특성과 자기적 성질을 연구하였다. 결정구조는 상온에서 입방정으로 정상 spinel 구조를 갖는 것으로 나타났다. 자기저항 실험결과 160K 부근 이하에서는 반도체적 전기전도 특성을 보이며, Curie 온도부근에서 최대자기저항 온도가 나타났다. Zn 조성값이 증가함에 따라 Jahn-Teller 효과에 의한 완화 현상이 증가되었으며, 전기 사중극자 이동값 역시 증가되고, 초미세 자기장값은 감소하였다. CMR 특성은 heterovalency에 의한 이중교환 상호작용이나, $Fe^{2+}$와 $Cr^{3+}$ 그리고 $Fe^{3+}$ 사이의 삼중교환 상호작용과는 다른 동적 Jahn-Teller 효과에 의한 도체-반도체전이와 절반 금속성 에너지 밴드구조에서 스핀전자 전이에 의하여 발생되는 것으로 예측된다.

• 한국자기학회지
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• 제23권2호
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• pp.43-48
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• 2013

Chalcogenide $Fe_{0.9}M_{0.1}Cr_2S_4$(M=Co, Ni, Zn)에 대하여 X-선 회절법, 자기저항측정, Mossbauer 분광법을 이용하여 CMR특성과 자기적 성질을 연구하였다. 10 at%의 M 치환에서는 상온에서 입방정으로 정상 spinel 구조를 갖는 것으로 나타났다. 자기저항 실험결과 $T_C$ 부근에서는 도체-반도체 전이의 특성을 보이며 최대자기저항 온도가 나타났다. M$\ddot{o}$ssbauer 분광 실험 결과에서 Fe에 대한 Ni 치환은 초교환 상호작용을 강화시키고 Jahn-Teller 효과에 의한 완화 현상의 심화를 보여준다. CMR 특성은 망간산화물의 $Mn^{3+}$와 $Mn^{4+}$ 사이의 이중교환상호작용과 다르게 동적 Jahn-Teller 효과와 관계된 polaron에 기인한 도체-반도체 전이 의한 것으로 해석된다.