• Title/Summary/Keyword: Fe-Co-Ni

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Evaluation of Surface Mechanical Properties of Electro-formed Fe-Ni-Co Thin Foil by Dynamic Nano-indentation and Finite Element Methods (Fe-Ni-Co 박판의 동적 나노 압침법과 유한 요소법에 의한 표면 기계적 특성 평가)

  • Gang, Bo-Gyeong;Choe, Yong
    • Proceedings of the Korean Institute of Surface Engineering Conference
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    • 2017.05a
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    • pp.124-124
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    • 2017
  • Fe-Ni-Co 합금 박막(<$100{\mu}m$)을 황화물계 용액에서 전주공정으로 제조하였다. XRF로 측정한 박판의 평균 조성은 Fe-34 wt.% Ni-3 wt.% Co 이다. AFM으로 측정한 표면 조도는 35.2 nm 이다. 표면의 나노 경도는 평균 5.4 GPa 이었다. Oliver 모델을 적용한 구리 박막의 탄성하강강성도는 약 75 이었다. Alekhin 모델을 적용한 구리 박막의 마찰계수, 피로한계는 각각 0.134, 0.027 이었다. 유한요소법으로 평가한 Berkovich 형 나노압침선단의 하중분포를 이차원 선형 및 비선형 해석하면 1 [mN]의 정적하중을 가한 Fe-Ni-Co 박막은 약 576 [mN]로 예측되었다. 압침선단의 하중집중정도는 표면탐침현미경으로 관찰한 압흔의 변형정도와 유사한 경향을 보였다.

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Exchange Coupling Field and Thermal Stability of Ni80Fe20/[Ir22/Mn78-Mn]/Co75Fe25 Multilayer Depending on Mn Content (Ni80Fe20/[Ir22/Mn78-Mn]/Co75Fe25 다층박막에서 Mn 함유량에 의존하는 교환결합력과 열적안정성)

  • Kim, B.K.;Lee, J.Y.;Kim, S.S.;Hwang, D.G.;Lee, S.S.;Hwang, J.Y.;Kim, M.Y.;Rhee, J.R.
    • Journal of the Korean Magnetics Society
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    • v.13 no.5
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    • pp.187-192
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    • 2003
  • The magnetic and thermal properties of NiFe/[IrMn-Mn]/CoFe with Mn additions have been studied. As-deposited CoFe pinned layers with [IrMn-Mn]layer had dominantly larger exchange biasing field ( $H_{ex}$) and blocking temperature ( $T_{b}$) than those with pure I $r_{22}$M $n_{78}$ used. The $H_{ex}$ and $T_{b}$ improved with 76.8-78.1 vol% Mn, but those of the NiFe/IrMn/CoFe dropped considerably with more addition of 0.6 vol % Mn. The average x-ray diffraction peak ratios of fcc [(111)CoFe, NiFe]/(111)IrM $n_3$ textures for the Mn inserted total vol of 75.5, 77.5, and 79.3% were about 1.4, 0.8, and 0.6, respectively. For the sample without Mn inserted layer, the $H_{ex}$ between IrMn and CoFe layers was almost zero, but it increased to 100 Oe after annealing of 250 $^{\circ}C$. For as-grown two multilayers samples with ultra-thin Mn layers of 77.5 and 78.7 vol %, the $H_{ex}$s were 259 and 150 Oe, respectively. In case of IrMn with 77.5 vol% Mn, the $H_{ex}$ was increased up to 475 Oe at 350 $^{\circ}C$ but decreased to 200 Oe at 450 $^{\circ}C$, respectively. The magnetic properties and thermal stabilities of NiFe/[IrMn-Mn]/CoFe multilayer were enhanced with Mn additions. In applications where higher $H_{ex}$ and $T_{b}$ are required, proper contents of Mn can be used. be used. used.

Structural Characterization of CoCrFeMnNi High Entropy Alloy Oxynitride Thin Film Grown by Sputtering (스퍼터링 방법으로 성장한 코발트크롬철망간니켈 고엔트로피 질산화물 박막의 구조특성)

  • Lee, Jeongkuk;Hong, Soon-Ku
    • Korean Journal of Materials Research
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    • v.28 no.10
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    • pp.595-600
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    • 2018
  • This study investigates the microstructural properties of CoCrFeMnNi high entropy alloy (HEA) oxynitride thin film. The HEA oxynitride thin film is grown by the magnetron sputtering method using nitrogen and oxygen gases. The grown CoCrFeMnNi HEA film shows a microstructure with nanocrystalline regions of 5~20 nm in the amorphous region, which is confirmed by high-resolution transmission electron microscopy (HR-TEM). From the TEM electron diffraction pattern analysis crystal structure is determined to be a face centered cubic (FCC) structure with a lattice constant of 0.491 nm, which is larger than that of CoCrFeMnNi HEA. The HEA oxynitride film shows a single phase in which constituting elements are distributed homogeneously as confirmed by element mapping using a Cs-corrected scanning TEM (STEM). Mechanical properties of the CoCrFeMnNi HEA oxynitride thin film are addressed by a nano indentation method, and a hardness of 8.13 GPa and a Young's modulus of 157.3 GPa are obtained. The observed high hardness value is thought to be the result of hardening due to the nanocrystalline microstructure.

Dependence of Coercivity and Exchange Bias by Thickness and Materials of Inserted Layer in [Pd/Co]5/X/FeMn Multilayer with Out-of-plane Magnetic Anisotropy (수직자기이방성을 갖는 [Pd/Co]5/X/FeMn 다층박막에서 삽입층 물질과 두께에 따른 교환바이어스와 보자력의 의존성)

  • Heo, Jang;Park, Dong-Hun;Kang, Wang-Son;Ji, Sang-Hun;Lee, Ky-Am
    • Journal of the Korean Magnetics Society
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    • v.18 no.5
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    • pp.185-189
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    • 2008
  • We observe the change of coercivity and exchange bias, depending on inserting material and thickness in a [Pd(0.6 nm)/$Co(0.2)]_5$/ FeMn(10) multilayer structure with perpendicular anisotropy. When 0.78 and 1.28 nm thick NiFe substitutes for Co in a $[Pd(0.6 nm)Co(0.2)]_4$/Pd(0.6)/NiFe(t)/FeMn(10) structure, we obtain the exchange bias of 360 Oe. In addition, when $Co_8Fe_2$ and $Co_9Fe_1$ are inserted for Co/FeMn interface, we obtain the exchange bias of 380 nm for a 0.68 nm thick $Co_8Fe_2$ and 580 Oe for a 0.52 nm thick $Co_9Fe_1$.

Comparison of the Heavy Metal Concentrations of the Soils and Plants at the Serpentine and Rhyolite Resions in Ulsan City (울산시의 사문암 및 유문암 지역 표토와 식물체의 중금속 함량 비교)

  • 김명희;민일식;송석환
    • Korean Journal of Environment and Ecology
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    • v.13 no.2
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    • pp.176-183
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    • 1999
  • 울산지역의 사문암과 유문암 토양 및 쑥과 참억새의 중금속 함량을 비교하기 위하여 중금속 농도를 분석한 결과 사문암 풍화토의 Ni, Cr 및 Co 함량은 매우 높았다. Ni은 1,483~1.524ppm, Cr은 372~435ppm, Co는 68~79ppm였으며, 유문암 풍화토의 Zn 함량은 222ppm으로 사문암 풍화토보다 높았다. 사문암 풍화토에서 생육하는 쑥의 중금속 함량은 Ni이 108~195ppm. Cr이 135~180ppm, Co가 10.2~22.5ppm으로 유문암 풍화토의 쑥보다 높았고, Zn은 유문암 토양 쑥에서 높았다. 참억새의 경우는 Ni, Cr, Co, As, Se, Mo 및 Fe 가 사문암 토양에서 높았고, Zn 흡수는 유문암 토양에서 많았다. 쑥의 중금속 함량은 대체적으로 지상부가 지하부보다 높았으나, 참억새의 경우는 지하부가 높은 경향을 나타내었다. 토양과 식물체(쑥과 참억새)의 중금속 함량을 비교해 보면 Ni, Cr, Co, As, Sc, Mo 및 Fe의 함량은 토양의 식물체보다 높았으나, 유문암 토양에 있는 쑥의 Zn 흡수는 토양보다 다소 높았다. 식물체의 Fe:Ni 비율은 유문암 토양보다는 사문암 토양이, 참억새보다는 쑥이 낮게 나타났다.

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Sliding Wear and Friction Behavior of Electro-Pressure Sintered Co-Fe and Co-Ni Compacts (통전가압 소결된 Co-Fe, Co-Ni 소결체의 미끄럼 마찰 및 마멸거동)

  • Kwon Yong Jin;Kim Tai-Woung;Kim Yong-Suk
    • Journal of Powder Materials
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    • v.11 no.6 s.47
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    • pp.451-461
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    • 2004
  • Dry sliding wear behavior of electro-pressure sintered Co-Fe and Co-Ni compacts was investigated. Pin-on-disk wear tests were performed on the sintered Co-Fe, Co-Ni disks against alumina $(Al_2O_3)$ and silica $(SiO_2)$ balls at various loads ranging from 3N to 12N. A constant sliding speed of 0.1m/sec was employed. Wear rate was calculated by dividing the weight loss of a specimen by the measured specific gravity and sliding dis-tance. Worn surfaces and cross-sections of the specimens were examined using an SEM and EDS to investigate wear mechanism of the compacts. The wear behavior of the compacts were discussed as a function of their com-position. Effects of mechancial properties of the compact as well as oxide layers formed on wearing surface on the wear were also discussed.

CHARACTERISTICS OF ELECTRICAL RESISTANCE IN MN-CO-NI-FE OXIDE (MN-CO-NI-FE 산화물의 전기저항특성)

  • YoungMinKim;ChaiSukYim;GoingYim
    • Journal of the Korean Geophysical Society
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    • v.4 no.4
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    • pp.257-266
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    • 2001
  • The properties of electrical resistance of Mn-Co-Ni-Fe oxide-based therrnistor with various Fe contents in sintering process at 1200 to 1400℃ for 4 hours in air atmosphere for fabricating therrnistor materials were investigated. The results were as follows: all samples showed single cubic spinel crystal structures in all region. The electrical conductivinity is the highlest thermistor sintered at 1300℃ for 4 hours. In general when the Fe content is increased except F-2, the resistivity increases and relatively the conductivity decreases. Particularly F-2 composition exhibited the highlest electrical conductivity(1.4x $10^-3$$Ω$cm) and relatively low B constant(2906K)

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Pt Thickness Dependence of Oscillatory Interlayer Exchange Coupling in [CoFe/Pt/CoFe]/IrMn Multilayers with Perpendicular Anisotropy

  • Lee, Sang-Suk;Choi, Jong-Gu;Kim, Sun-Wook;Hwang, Do-Guwn;Rhee, Jang-Roh
    • Journal of Magnetics
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    • v.10 no.2
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    • pp.44-47
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    • 2005
  • The oscillatory interlayer exchange coupling (IEC) has been shown in pinned $[CoFe/Pt(t_{pt})/CoFe]/IrMn$ multi-layers with perpendicular anisotropy. The period of oscillation corresponds to about 2 monolayers of Pt. The oscillatory behavior of IEC depending on the nonmagnetic metallic Pt thickness is thought to be related the antiferromagnetic ordering induced by IrMn layer. Oscillatory IEC as function of insulating NiO thickness has been observed in $[Pt/CoFe]_4/NiO(t_{NiO})/[CoFe/Pt]_4$ multilayers. The effect of N (number of bilayer repeats) upon the magnetic property of [Pt/CoFe]N/IrMn is also studied.

Magnetization Switching of MTJs with CoFeSiB/Ru/CoFeSiB Free Layers (CoFeSiB/Ru/CoFeSiB 자유층을 갖는 자기터널 접합의 스위칭 자기장)

  • Lee, S.Y.;Lee, S.W.;Rhee, J.R.
    • Journal of the Korean Magnetics Society
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    • v.17 no.3
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    • pp.124-127
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    • 2007
  • Magnetic tunnel junctions (MTJs), which consisted of amorphous CoFeSiB layers, were investigated. The CoFeSiB layers were used to substitute for the traditionally used CoFe and/or NiFe layers with an emphasis given on understanding the effect of the amorphous free layer on the switching characteristics of the MTJs. CoFeSiB has a lower saturation magnetization ($M_s\;:\;560\;emu/cm^3$) and a higher anisotropy constant ($K_u\;:\;2800\;erg/cm^3$) than CoFe and NiFe, respectively. An exchange coupling energy ($J_{ex}$) of $-0.003\;erg/cm^2$ was observed by inserting a 1.0 nm Ru layer in between CoFeSiB layers. In the Si/$SiO_2$/Ta 45/Ru 9.5/IrMn 10/CoFe 7/$AlO_x$/CoFeSiB 7 or CoFeSiB (t)/Ru 1.0/CoFeSiB (7-t)/Ru 60 (in nm) MTJs structure, it was found that the size dependence of the switching field originated in the lower $J_{ex}$ using the experimental and simulation results. The CoFeSiB synthetic antiferromagnet structures were proved to be beneficial for the switching characteristics such as reducing the coercivity ($H_c$) and increasing the sensitivity in micrometer size, even in submicrometer sized elements.

Preparation and Properties of Co$_{9-x}M_xS_8$(M = Ni, Rh, Ru, and Fe)

  • Kim, Kwan
    • Bulletin of the Korean Chemical Society
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    • v.7 no.2
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    • pp.102-105
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    • 1986
  • Samples with the nominal composition of $Co_{9-x}M_xS_8$(M = Ni, Rh, Ru, and Fe) were prepared, and their magnetic properties were measured. X-ray diffraction analysis showed that small amount of the elements Ni, Rh, and Fe could be incorporated into $Co_9S_8$ forming a homogeneous ${\pi}$-phase, whereas the Ru-incorporated sample could not be prepared in a single phase. The lattice parameter was observed to increase as other elements were incorporated into $Co_9S_8$. Samples incorporated with the elements of Ni, Rh, and Ru showed Pauli-paramagnetism while the Fe-incorporated sample exhibited weak ferromagnetism. The values of magnetic susceptibility for the Ni, Rh, Ru-incorporated samples were nearly the same as that of pure $Co_9S_8$.