• 한국세라믹학회:학술대회논문집
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• 한국세라믹학회 2000년도 춘계총회,특별강연,심포지움,연구발표회
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• pp.88.2-88.2
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• 2000

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1996년도 춘계연구발표회 논문개요집
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• pp.82-83
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• 1996

• 한국세라믹학회:학술대회논문집
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• 한국세라믹학회 2000년도 추계총회,초청강연,특별강연,연구발표회
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• pp.68.1-68
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• 2000

• 한국세라믹학회:학술대회논문집
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• 한국세라믹학회 2000년도 추계총회,초청강연,특별강연,연구발표회
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• pp.157.2-157
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• 2000

• 한국자기학회지
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• 제9권6호
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• pp.278-284
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• 1999

Mn-Zn ferrites에 TiO2가 첨가될 때 전력손실, 밀도, 초기투자율, 저항, 그리고 미세구조의 변화를 관찰하였다. 첨가량이 증가함에 따라 밀도는 증가했지만, 초기투자율은 감소하였다. TiO2의 첨가에 따라 electron hopping을 일으키는 활성화에너지와 전기저항이 증가하였다. 115$0^{\circ}C$에서 소결한 TiO2를 1.5 wt% 첨가한 시편은 1 MHz, 25 mT, 8$0^{\circ}C$에서 83 mW/㎤의 전력손실을 나타내었다. 그러나 120$0^{\circ}C$에서 소결할 때는 과대입성장이 발생하여 같은 측정 조건에서 1168 mW/㎤의 전략손실을 얻었다.

• Journal of electromagnetic engineering and science
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• 제5권4호
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• pp.161-165
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• 2005

We prepared Mn-Zn ferrite Electromagnetic(EM) wave absorbers. The Mn-Zn ferrite EM wave absorbers were coated with Sr ferrite powders and $Al(OH)_3$ powders. The coated Mn-Zn ferrite EM wave absorbers show improved absorption compared with non-coated Mn-Zn EM wave absorbers.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1998년도 춘계연구발표회 논문개요집
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• pp.68-69
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• 1998

• 한국재료학회지
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• 제5권8호
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• pp.1026-1034
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• 1995

저손실 망간징크 페라이트에서 CaO-SiO$_2$첨가는 입계에 높은 전기저항층을 형성시켜 와류에 의한 손실을 감소시키는 것으로 알려져 있다. 본 실험에서는 Nb$_2$O$_{5}$ 를 제 3의 첨가제로 사용하여 저손실 망간징크 페라이트에서의 전자기적 물성변화를 관찰하였다. Nb$_2$O$_{5}$ 300ppm 이상 첨가시 부분적인 과대입자 성장이 관찰되었으며, 200ppm 첨가시 CaO-SiO$_2$만 첨가한 시편에 비하여 밀도가 증가하였다. Nb$_2$O$_{5}$ 첨가시에는 100ppm 이하의 SiO$_2$첨가에서 우수한 전력손실 특성이 나타났으며, 고온 소결시 Nb$_2$O$_{5}$-CaO를 첨가한 시편에서 낮은 전력손실을 나타내었다.

• 한국세라믹학회지
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• 제28권7호
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• pp.556-560
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• 1991

The behavior of Ni-Zn ferrite/Mn-Zn ferrite composite electromagnetic absorber was investigated. The imaginary part of complex permeability of the composite was higher than that of either ferrite alone at all frequency range (50∼1400MHz) studied. The difference, which was pronounced in low frequency range, was reached the maximum value when the composite consisted of constituent ferrites with equal amount. Since the thickness in inversely proportional to the imaginary part of complex permeability for the ferrite absorber, it was possible to reduce the thickness of electromagnetic absorber by employing a composite of two different ferrites.

• Journal of Magnetics
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• 제21권3호
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• pp.308-314
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• 2016

Cobalt-, zinc-, and nickel-zinc-substituted nano-size manganese ferrite powders, $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, $Mn_{0.8}Zn_{0.2}Fe_2O_4$ and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$, were fabricated using a sol-gel method, and their crystallographic and magnetic properties were subsequently studied. The $MnFe_2O_4$ ferrite powder annealed at temperatures above 523 K exhibited a spinel structure, and the particle size increased as the annealing temperature increased. All ferrites annealed at 773 K showed a single spinel structure, and the lattice constants and particle size decreased with the substitution of Co, Zn, and Ni-Zn. The $M{\ddot{o}}ssbauer$ spectrum of the $MnFe_2O_4$ ferrite powder annealed at 523 K only showed a doublet due to its superparamagnetic phase, and the $M{\ddot{o}}ssbauer$ spectra of the $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, and $Mn_{0.8}Zn_{0.2}Fe_2O_4$ ferrite powders annealed at 773 K could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. However, the $M{\ddot{o}}ssbauer$ spectrum of the $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$ ferrite powder annealed at 773 K consisted of two Zeeman sextets and one quadrupole doublet due to its ferrimagnetic and paramagnetic behavior. The area ratio of the $M{\ddot{o}}ssbauer$ spectra could be used to determine the cation distribution equation, and we also explained the variation in the $M{\ddot{o}}ssbauer$ parameters by using this cation distribution equation, the superexchange interaction and the particle size. Relative to pure $MnFe_2O_4$, the saturation magnetizations and coercivities were larger in $Mn_{0.8}Co_{0.2}Fe_2O_4$ and smaller in $Mn_{0.8}Zn_{0.2}Fe_2O_4$, and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$. These variations could be explained using the site distribution equations, particle sizes and magnetic moments of the substituted ions.