• 한국자기학회:학술대회 개요집
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• 한국자기학회 2004년도 하계학술연구발표회 논문개요집
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• pp.200-200
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• 2004

• 한국주조공학회지
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• 제24권6호
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• pp.356-365
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• 2004

Mechanical properties and microstructures of the Ni-AI-Fe and Ni-AI-Fe-(B, Zr) alloys which containing $10{\sim}30at$.%Fe, 0.1at.%B and/or 0.1at.%Zr have been investigated. The experimental results showed that the microstructures of Ni25Al were changed from a single phase ${\gamma}$ to dual phase ${\gamma}$ and ${\beta}$ by addition of 27at.%Fe. Ni45Al, however, kept the single ${\beta}$ phase even though Fe was added upto 30at.%. The hardness of Ni25Al were increased from $H_RB$ 70 to $H_RC$ 39 by addition of 27at.%Fe. In the case of Ni45Al which have $H_RC$ 37, the hardness was decreased by lOat.%Fe addition, but increased with 30at.%Fe. The yield strength and ultimate compressive strength in the compressive test have showed a similar trend with the hardness change. The strain to fracture was 14% at maximum and achieved in Ni25Al-27at.%Fe and Ni25Al-27at.%Fe-0.1 at.%B alloys. The Ni45Al showed a relatively low strain to fracture as 4%. The impact absorption energy of Ni25Al increased from 0.74 kg-m to 1.81 kg-m by addition of 27at.%Fe. In case of Ni45Al, the addition of lOat.%Fe and lOat.%Fe with small amounts of Band Zr did not change significantly the impact absorption energy of 0.60 kg-m, whereas the addition of 30at.%Fe with small amounts of B and Zr increased it slightly. In fracture tests, both of two basic materials showed the same intergranular fracture but by adding Fe it changed to the cleavage fracture mode or co-existing of cleavage and intergranular fractures.

• 한국결정성장학회지
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• 제22권5호
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• pp.218-222
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• 2012

FeNi alloy nanofibers have been prepared by an electrospinning process followed by air-calcination and H2 reduction to develop electromagnetic (EM) wave absorbers in the giga-hertz (GHz) frequency range. The thermal behavior and phase and morphology evolution in the synthetic processes were systematically investigated. Through the heat treatments of calcination and H2 reduction, as-spun PVP/FeNi precursor nanofiber has been stepwise transformed into nickel iron oxide and FeNi phases but the fibrous shape was maintained perfectly. The FeNi alloy nanofiber had the high aspect ratio and the average diameter of approximately 190 nm and primarily composed of FeNi nanocrystals with an average diameter of ~60 nm. The FeNi alloy nanofibers could be used for excellent EM wave absorbing materials in the GHz frequency range because the power loss of the FeNi nanofibers increased up to 20 GHz without a degradation and exhibited the superior EM wave absorption properties compared to commercial FeNi nanoparticles.

• 한국자기학회지
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• 제6권5호
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• pp.329-333
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• 1996

Cu/(NiFe/Ni/NiFe) 금속다층막을 Si(100), Si(111), $4^{\circ}\;tilt-cut\;Si(111)$, slide glass등의 기판 위에 형성하여 자기저항 특성 및 자기이방성을 고찰하였다. $50\;{\AA}$의 Cu를 바닥층으로 사용한 경우 $4^{\circ}\;tilt-cut\;Si(111)$ 기판 위에서 면내 일축 자기이방성을 보였으며 다른 기판 위에서는 자기이방성을 보이지 않았다. 바닥층이 없는 경우나 NiFe, Ni등을 바닥층으로 사용한 경우 $4^{\circ}\;tilt-cut\;Si(111)$ 기판 위에서 자기이방성은 나타나지 않았으며, Cu 바닥층을 증착하기 전 NiFe를 $10\;{\AA}$ 증착하고 형성한 금속다층막의 경우도 면내 자기이방성이 나타나지 않았다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.304-304
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• 2011

We investigated the effect of different spin direction of anti-ferromagnetic layer on the magnetic properties of ferromagnetic layer in Fe-NiO and Fe-CoO bi-layer systems. For Fe-NiO system, we prepared the clean MgO(001) surface half-covered with 20 nm Ag films as a substrate for magnetic layers. Then we grew NiO wedge layers on the substrate, and added 8 monolayer(ML) Fe layers on the wedge layer. We examined magnetic properties of the bi-layer system using the surface magnetic optical Kerr effect(SMOKE) and X-ray magnetic linear dichroism(XMLD). From SMOKE measurement we observed the coercivity enhancement due to the set-up of anti-ferromagnetic order of NiO films in both of the Fe/NiO/MgO(001) and Fe/NiO/Ag/MgO(001) system. The most remarkable results in our observation is that the coercivity enhancement of Fe/NiO/Ag/MgO(001) is much larger than that of Fe/NiO/MgO(001). XMLD experiments confirmed the out-of-plane spin direction of NiO layers in Fe/NiO/MgO(001) and in-plane spin-direction of NiO layers in Fe/NiO/Ag/MgO(001), and we concluded that the origin of large enhancement of coercivity is due to the strong parallel coupling between Fe layers and NiO layers. We also confirmed that this strong parallel coupling maintained across the thin Ag layer inserted between Fe and NiO layers. For Fe-CoO system, we prepared Fe/CoO/Ag(001) and Fe/CoO/MnO(001) systems and observed much larger coercivity enhancement in Fe/CoO/Ag(001).

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1997년도 추계연구발표회 논문개요집
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• pp.28-29
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• 1997

• 한국자기학회지
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• 제12권6호
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• pp.212-217
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• 2002

비자성층을 사이에 둔 두 강자성층의 보자력 차이를 이용하여 거대자기저항특성을 나타내는 Ta/CoFe/Cu/NiFe/Ta 구조의 pseudo 스핀밸브를 DC 마그네트론 스퍼터링 방법으로 제조하였다. Ta/CoFe/Cu/NiFe/Ta 구조에서 CoFe층의 두께 변화에 따른 자화 특성 및 자기저항 특성을 조사하였으며, 이 구조에서 CoFe층의 두께가 60 $\AA$일 때 자기저항비는 3.82%이고 CoFe층과 NiFe층 사이의 보자력 차이는 27.4 Oe이다. Ta/CoFe/Cu/NiFe/Ta 구조를 갖는 pseudo 스핀밸브에서 CoFe층과 NiFe층의 보자력 차이는 CoFe층의 두께가 20 $\AA$에서 40 $\AA$까지 증가함에 따라 증가하였으며 40 $\AA$ 이상에서는 감소하였다. 이와 같은 결과는 박막의 결정성 및 포화 자기변형(λ$_{s}$)의 변화에 의한 것으로 판단된다. Cu층과 NiFe층 사이에 CoFe층을 삽입한 Ta/CoFe/Cu/NiFe/Ta 구조에서 삽입층인 CoFe층의 두께 변화에 따른 자화특성 및 자기저항 특성을 조사한 결과 CoFe두께가 10$\AA$시 자기저항비가 6.7 %이며. 삼층막 구조 보다 자기저항비가 약 1.5배 이상 증가함을 알 수 있었다.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2000년도 International Symposium on Magnetics The 2000 Fall Conference
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• pp.303-304
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• 2000

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1998년도 추계연구발표회 논문개요집
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• pp.22-23
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• 1998

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1998년도 추계연구발표회 논문개요집
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• pp.20-21
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• 1998