• 한국수소및신에너지학회논문집
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• 제14권4호
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• pp.298-304
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• 2003

The thermal behavior of $NiFe_2O_4$ prepared by a solid-state reaction was investigated for $H_2$ generation by the thermochemical cycle. The reduction of $NiFe_2O_4$ started from $800^{\circ}C$, and the weight loss was 0.2-0.3 wt% up to $1000^{\circ}C$. In the $H_2O$ decomposition reaction, $H_2$ was generated by oxidation of reduced $NiFe_2O_4$. The crystal structure of $NiFe_2O_4$ maintained during the redox reaction of 5 cycles. From this observation, the lattice oxygen in $NiFe_2O_4$ is released without the structural change during the thermal reduction and oxygen deficient $NiFe_2O_4$ can be restored to the spinel structure of $NiFe_2O_4$.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2000년도 추계학술대회 논문집
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• pp.355-358
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• 2000

Magnetoresistance changes of NiFe thin films were investigated as a function of deposition temperature. DC magnetron sputtering was employed to fabricate Ta/NiFe(t)/Ta thin films on Si(001) substrates with in-situ field or with no-field. The thickness(t) of NiFe films was a range of 4 to 15nm. Substrate temperature was a range of 30 to 400$^{\circ}C$. MR measurement was carried out as a function of angle $\theta$, between external field and current direction. MR ratio increased with increasing substrate temperature, also, max. MR ratio was observed in samples deposited at 300$^{\circ}C$. With increasing upto 400$^{\circ}C$, MR ratio was rapidly decreased in the case of thinner NiFe films. In non-field deposited NiFe films, both angle $\theta$=0, 90。, there was no significant change in MR curves. However, MR curves of in-situ field deposited NiFe films were different in both angles $\theta$=0 and 90。

• 한국표면공학회지
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• 제36권6호
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• pp.455-460
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• 2003

Microstructural and magnetic properties of nanocrystalline Fe-46 wt%Ni and Fe-36 wt%Ni alloys were investigated. Alloys were prepared by the electrodeposition process. The electrolytes were iron sulfate/nickel chloride-based and iron chloride/nickel sulfamate-based solutions. Fe-46 wt%Ni alloy was FCC structure with grain size of 10 nm, but FCC and BCC phases were found in Fe-36 wt%Ni alloy and its grain size was smaller. Effective permeability of Fe-36 wt%Ni alloy was higher than that of Fe-46 wt%Ni alloy in the high frequency range because of large electrical resistivity and small eddy current loss resulted from grain size decrease. Up to $300^{\circ}C$ of annealing temperature, grain growth of Fe-Ni alloys slowly occured. Conversely, annealing above $450^{\circ}C$ led to a drastic grain growth. In that case, effective permeability was decreased at the temperature lower than $300^{\circ}C$ but at $300^{\circ}C$ or higher effective permeability was increased. At the high frequency of 1 MHz, electrodeposited Fe-Ni alloys had higher effective permeability with an decrease in the grain size.

• 한국표면공학회지
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• 제36권6호
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• pp.461-465
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• 2003

The microstructures and magnetic properties of electrodeposited Fe-45 wt%Ni-P alloys have been investigated. The structures of electrodeposited Fe-45 wt%Ni alloy was FCC i.e. ${\gamma}$ phase and the size of crystallite was 10 nm. The structure of electrodeposited Fe-45 wt%Ni-1 wt%P alloy showed ${\gamma}$ phase and 7 nm sized nanocrystalline. The electrodeposited Fe-45 wt%Ni-P alloys containing 2∼3 wt% of P exhibited ${\gamma}$ ＋ $\alpha$ dual phases. The electrodeposited Fe-45 wt%Ni-P alloys above 3.5 wt% showed an amorphous structure. P in the alloys acted grain refining and phase changing element. The resistivity of the electrodeposited alloys increased with P contents. Effective permeability at high frequency (above 1 MHz) increased with P contents up to 2 wt% and this was ascribed to the easier magnetization rotation owing to the reduction of eddy current. Effective permeability decreased with P contents above 3 wt% and this was ascribed to the transformation of the ferromagnetism of Fe-45 wt%Ni alloy gradually into paramagnetism with the introduction of P into the electrodeposited alloy matrix.

• Corrosion Science and Technology
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• 제22권6호
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• pp.478-483
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• 2023

This study examined the corrosion behavior of bimetal materials composed of Fe-Ni alloy and Fe-Ni-Mo alloy, both suitable for use in electromagnetic switches. Electrochemical polarization and weight loss measurements revealed that, in contrast to Fe-Ni alloy, which exhibited pseudo-passivity behavior, Fe-Ni-Mo alloy had higher anodic current density, displaying only active dissolution and greater weight loss. This indicated a lower corrosion resistance in the Fe-Ni-Mo alloy. Equilibrium calculations for the phase fraction of precipitates suggested that the addition of 1 wt% Mo may lead to the formation of second-phase precipitates, such as Laves and M₆C, in the γ matrix. These precipitates might degrade the homogeneity of the passive film formed on the surface, leading to localized attacks during the corrosion process. Therefore, considering the differences in corrosion kinetics between these bimetal materials, the early degradation caused by galvanic corrosion should be prevented by designing a new alloy, optimizing heat treatment, or implementing periodic in-service maintenance.

• Journal of Magnetics
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• 제21권1호
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• pp.40-45
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• 2016

Nickel substituted nano-sized ferrite powders, $Co_{1-x}Ni_xFe_2O_4$, $Mn_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ($0.0{\leq}x{\leq}0.2$), were fabricated using a sol-gel method, and their crystallographic and magnetic properties were subsequently compared. The lattice constants decreased as quantity of nickel substitution increased, while the particle size decreased in $Co_{1-x}Ni_xFe_2O_4$ ferrite but increased for the $Mn_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites. For the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-x}Ni_xFe_2O_4$ ($0.0{\leq}x{\leq}0.2$) ferrite powders, the $M{\ddot{o}}ssbauer$ spectra 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 $Mn_{0.8}Zn_{0.1}Ni_{0.1}Fe_2O_4$ consisted of two Zeeman sextets and one single quadrupole doublet due to the 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 explain the variation in the $M{\ddot{o}}ssbauer$ parameters by using this cation distribution equation, the superexchange interaction and the particle size. The saturation magnetization decreased in the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites but increased in the $Mn_{1-x}Ni_xFe_2O_4$ ferrite with nickel substitution. The coercivity decreased in the $Co_{1-x}Ni_xFe_2O_4$ and $Mn_{1-2x}Zn_xNi_xFe_2O_4$ ferrites but increased in the $Mn_{1-x}Ni_xFe_2O_4$ ferrite with nickel substitution. These variations could thus be explained by using the site distribution equations, particle sizes and spin magnetic moments of the substituted ions.

• 한국자기학회지
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• 제9권1호
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• pp.41-47
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• 1999

DC magnetron sputtering 방법으로 Corning glass 기판 위에 기저층을 Cr과 Ta로 바꾸어가면서 보자력이 다른 Ni81Fe19와 CoFe(Co)를 이용하여 buffer;[FeNi/Cu/CoFe(Co)/Cu]N의 형태로 spin-valve 다층박막을 제작하여 자기저항비의 기저층 종류와 두께, 비자성층 Cu층 두께, 연자성층 NiFe층 두께, 사이층 박막 반복 적층횟수, 기판온도 및 열처리 온도 의존성을 조사하였다. 제작된 시료의 자기저항비는 4탐침법으로 측정하였으며 이들의 구조, 자기적 성질을 조사하기 위해 X-선 회절분석, 시료진동형 자기계(VSM) 분석을 하였다. Cr기저층 두께가 50$\AA$, Cu 두께 50$\AA$, NiFe 및 Co 두께가 각각 20$\AA$이며 사이층 박막 반복 적층횟수 10인 경우에 기판온도가 9$0^{\circ}C$일 때 극대 자기저항비 및 보자력은 각각 7.5% 및 140 Oe를 보이다가 기판온도 상승에 따라 감소하였다. 자기장 감응도(MR slope)는 열처리 온도 15$0^{\circ}C$까지는 0.25%/Oe을 유지하다가 20$0^{\circ}C$에서는 0.03%/Oe로 감소하였으며 열안정성을 결정하는 주요한 요인은 NiFe 자성층의 연자기 특성 저하라는 것을 확인할 수 있었다.

• 한국세라믹학회지
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• 제28권4호
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• pp.305-314
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• 1991

This study was conducted to research the formation and the color development of NiO-ZnO-Fe2O3-TiO2-SnO2 system for the purpose of synthesizing the spinel pigments which are stable at high temperature. After preparing ZnO-Fe2O3 as a basic composition, {{{{ chi }}NiO.(l-{{{{ chi }})ZnO.Fe2O3 system, {{{{ chi }}NiO.(l-{{{{ chi }})ZnO.TiO2 system, and {{{{ chi }}NiO.(l-{{{{ chi }})ZnO.SnO2 system were prepared with {{{{ chi }}=0, 0.2, 0.5, 0.7, 1 mole ratio respectively. The manufacturing was carried out at 128$0^{\circ}C$ for 30 minutes. The reflectance measurement and the X-ray analysis of these specimens were carried out and the results were summarized as follows. 1. In the specimens which included NiO, it was difficult for the spinel structure to be formed. 2. As increasing the contents of NiO and Fe2O3, all the groups which were yellow or green colored changed to brown. 3. NiO-ZnO-Fe2O3 system and NiO-ZnO-TiO2 system formed the spinel structure and the illmenite structure appeared in NiO-TiO2 system.

• 한국자기학회지
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• 제18권5호
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• pp.180-184
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• 2008

이온빔 증착법으로 제작한 코닝유리(Corning glass)/Ta(5 nm)/NiFe(7 nm)/FeMn(25 nm)/Ta(5 nm) 다층박막 구조에서 반강자성체 FeMn층 증착시 인가한 일축 이방성 자기장 방향에 따른 강자성체 NiFe층의 자화 스핀배열 의존성을 조사하였다. NiFe층과 FeMn 층 증착시 인가한 자기장 방향을 달리한 각도는 각각 $0^{\circ},\;45^{\circ},\;90^{\circ}$였다. 용이축 MR(magnetoresistaice) 곡선으로부터 얻은 교환결합세기(Hex)는 증착 자기장 각도가 $45^{\circ}$일 때 40 Oe로, $90^{\circ}$일 때는 거의 0 Oe로 감소하였다. 반면에 곤란축 MR 곡선으로부터 얻은 $H_{ex}$ 값은 증착 자기장 각도가 $45^{\circ}$일 때 35 Oe로, 90o일 때는 79 Oe로 증가하였다. 강자성체 층의 용이축과 반강자성체 층의 일축 이방성 방향이 $90^{\circ}$ 차이가 나는 계면에서도 FeMn층이 NiFe층의 자기모멘트 스핀방향을 회전시켜 교환결합 이방성 효과가 발생함을 알 수 있었다.

• 한국자기학회지
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• 제14권6호
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• pp.228-231
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• 2004

Ta(5 nm)/NiFe(11 nm)/FeMn(16 nm) Ta(5 nm)과 Ta(5 nm)/NiFe(11 run)/FeMn(16 nm)/NiFe(7 nm)/Ta(5 nm) 다층박막구조를 제작하여, Laser의 power, 조사 위치, 자장의 방향에 따라 자기저항(MR)비와 교환결합력(H$_{ex}$) 자기적 특성을 연구하였다. Laser 열처리는 power를 440 mW까지 증가시키면서 FeMn/NiFe 이중박막을 15분 씩 Laser로 조사하여, 200 mW에서부터 음의 자기장에서 자기저항곡선의 피크가 발생하기 시작하였다. 400 mW까지 증가시키면서 양의 자기장에서 자기저항곡선의 MR비와 H$_{ex}$:가 각각 0.9%에서 0.1%로, 87 Oe에서 76 Oe로 감소하였고, 음의 자기장 피크에서는 MR비와 H$_{ex}$가 모두 증가하였다. 또한 NiFe/FeMn/NiFe삼중박막에서도 같은 결과를 얻었다. 300 mA로 laser열처리한 면적을 증가시켰을 때 자기저항곡선이 positive 피크는 감소하고 negative 피크는 증가하였다. 이러한 Laser 열처리효과에 의해 결과적으로 교환결합된 박막구조의 국소적 자화반전을 가능하게 하였다.