• 한국자기학회지
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• 제7권6호
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• pp.293-298
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• 1997

기계적합금법으로 Fe$_{5}$Si$_{x}$B$_{5-x}$ 분말을 제조하고, Si 치환에 따른 합성상의 변화 및 합성분말의 자기적 성질을 XRD, TEM, Mossbauer spectroscopy, VSM 등으로 조사하였다. 각 출발 원소들은 milling 초기에 .alpha. -Fe 구조로 고용되어 비정질(amorphous) 상태로 되며, 기계적합금화가 진행됨에 따라 최종 안정상이 석출되었다. Fe$_{5}$B$_{5}$ 조성의 경우(x=0) 250시간 볼밀 처리한 후 800 .deg. C에서 2시간 열처리하면 FeB와 Fe$_{2}$B 상이 혼재된 구조가 얻어 진다. B의 일부를 Si으로 치환하면 Fe$_{2}$B 상의 생성이 억제되는 반면에 여분의 Si이 Fe$_{5}$SiB$_{2}$, Fe$_{2}$Si$_{0.4}$B$_{0.6}$ 상 및 상자성 상을 형성한다. FeB 상은 800 .deg. C에서 열처리한 후에도 결정성이 높지 않아서 넓은 범위의 초미세자장 값을 갖는 반면에, 다른 상들은 결정화가 이루어져 일정한 초미세자장 값을 보였다. 포화자화 값은 Fe$_{2}$B 상이 가장 많이 함유된 Fe$_{5}$B$_{5}$ 조성에서 가장 크게 나타났다.다.

• 한국재료학회지
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• 제14권3호
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• pp.218-223
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• 2004

P-type $\beta$-FeSi$_2$ with a nominal composition of $Fe_{0.92}Mn_{0.08}Si_2$ powders has been produced by mechanical alloying process. As-milled powders were spray dried and consolidated by atmospheric plasma thermal spraying as a rapid sintering process. As-milled powders were of metastable state and fully transformed to $\beta$-$FeSi_2$ phase by subsequent isothermal annealing. However, as-thermal sprayed $Fe_{0.92}Mn_{0.08}Si_2$ consisted of untransformed mixture of $\alpha$-$Fe_2Si_{5}$ and $\varepsilon$-FeSi phases. Isothermal annealing has been carried out to induce transformation to the thermoelectric semiconducting $\beta$-$FeSi_2$ phase. Isothermal annealing at $845^{\circ}C$ in vacuum gradually led to the thermoelectric semiconducting $\beta$-$FeSi_2$ phase transformation, but some residual metallic $\alpha$ and $\varepsilon$ phases were unavoidable even after prolonged annealing. Thermoelectric properties of $\beta$-$FeSi_2$ materials before and after isothermal annealing were evaluated. Seebeck coefficient increased and electric conductivity decreased with increasing annealing time due to the phase transition from metallic phases to semiconducting phases. Thermoelectric properties showed gradual increment, but overall properties appeared to be inferior to those of vacuum hot pressed specimens.

• 한국자기학회지
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• 제20권1호
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• pp.13-17
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• 2010

연자기 특성이 우수한 것으로 잘 알려진 Fe-6.5 % Si 합금을 분말로 제작하여 성형한 Fe-6.5 % Si 압분코어에서도 좋은 특성을 얻을 수 있는 지를 확인하기 위해 Fe-3, 4.2 그리고 6.8 % Si 압분코어를 각각 제작하여 교류와 직류 자기특성, 미소경도 등을 분석하였다. 실리콘 함량이 증가할수록 와전류손실은 감소하나 이력손실은 증가하여 Fe-6.8 % Si에서 최소손실을 얻을 수 없었다. 또한 실리콘함량이 증가할수록 코어의 전기비저항과 분말입자의 미소경도는 지속적으로 증가하였으며 이 때문에 충진율은 감소하였다. B2와 $DO_3$상이 Fe-6.8 % Si 분말에서만 생성된 것을 확인할 수 있었으며, 6.8 % Si보다 낮은 실리콘 함량에서 코어손실이 더 낮은 것을 절연체와 분말입자의 비저항 비율, 미소경도변화에 따른 충진율 저하와 반자장 효과 등으로 설명할 수 있었다.

• 한국자기학회지
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• 제5권4호
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• pp.281-286
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• 1995

Hexaferrite $Ba_{0.25}Sr_{0.75}Fe_{12}O_{19}$에 $SiO_{2}$를 첨가한 쉬트자석의 자기적 성질의 변화를 연구하기 위해 X-선 회절 실험, 뫼스바우어 분광실험, 자기모멘트 측정실험 등을 하였다. 쉬트자석은 Dr. Blade 방법에 의해 제조되었고, 결정구조는 마그네토플럼바이트 M-type 육방결정구조이다. 첨가제 농도에 따른 격자상수의 변화는 거의 없으나, $SiO_{2}$가 2.0 wt.% 이상부터 ${\alpha}-Fe_{2}O_{3}$ 의 상이 나타나기 시작했다. 이성질체 이동값은 Fe이온들이 3가 임을 나타낸다. $SiO_{2}$의 증가에 따라 Curie 온도는 감소함을 보였다. 이것은 $Si^{4+}$가 12k-site $Fe^{3+}$의 자리를 차지함으로써 Fe-O-Fe의 초교환상호작용에 의한 원자간 거리와 양이온 사이의 각이 변함에 따른 것이다. ${\alpha}-Fe_{2}O_{3}$의 상은 $Si^{4+}$가 12k-site $Fe^{3+}$의 자리를 차지함으로 치환된 $Fe^{3+}$에 의해 나타난 것이다. 자기모멘트측정으로 부터 $SiO_{2}$를 첨가한 $Ba_{0.25}Sr_{0.75}Fe_{12}O_{19}$ 쉬트자석은 보자력 $H_{c}$, 포화자화 $M_{s}$, 잔류자화 $M_{r}$이 양이온 치환보다는 미세구조변화에 더 의존함을 알았다.

• 한국주조공학회지
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• 제33권2호
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• pp.55-62
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• 2013

Effect of Fe and Mn contents on the castability of Al-4wt%Mg-0.9wt%Si system alloy has been studied. According to the analysis of cooling curve for Al-4wt%Mg-0.9wt%Si-0.3wt%Fe-0.3/0.5wt%Mn alloy, ${\alpha}-Al_{15}(Fe,Mn)_3Si_2$ and ${\beta}-Al_5FeSi$ phases crystallized above eutectic temperature of $Mg_2Si$. Therefore, these phases affected both the fluidity and shrinkage behaviors of the alloy during solidification. As Fe and Mn contents of Al-4wt%Mg-0.9wt%Si system alloy increased from 0.1 wt% to 0.4 wt% and from 0.3 wt% to 0.5 wt% respectively, the fluidity of the alloy decreased by 26% and 33%. When Fe content of the alloy increased from 0.1 wt% to 0.4 wt%, 23% decrease of macro shrinkage and 19% increase of micro shrinkage appeared. Similarly, Mn content of the alloy increased from 0.3 wt% to 0.5 wt%, 11% decrease of macro shrinkage and 14% increase of micro shrinkage appeared. Judging from the castability of the alloy, Al-4wt%Mg-0.9wt%Si alloy with low content of Fe and Mn, 0.1 wt% Fe and 0.3 wt% Mn, is recommendable.

• 한국주조공학회지
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• 제33권6호
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• pp.233-241
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• 2013

Effect of Fe and Mn contents on the castability of Al-9wt%Si-xMg-yFe-zMn alloy has been studied. The alloy was composed of ${\alpha}$-Al phase, Al+eutectic Si phase, ${\beta}$-Al5FeSi compound and chinese script ${\alpha}$-$Al_{15}(Mn,Fe)_3Si_2$ compound. ${\beta}$-$Al_5FeSi$ and ${\alpha}$-$Al_{15}(Mn,Fe)_3Si_2$ compounds assumed to effect the fluidity and shrinkage behaviors of the alloy during solidification due to the crystallization of ${\alpha}$-$Al_{15}(Fe,Mn)_3Si_2$ and ${\beta}$-$Al_5FeSi$ compounds above eutectic temperature. As Fe and Mn contents of Al-9wt%Si-0.3wt%Mg system alloy increased from 0.15wt% to 0.6wt% and from 0.3wt% to 0.7wt%, fluidity of the alloy decreased by 5.7% and 3.3%, respectively. And as Mg content of Al-9wt%Si-0.45wt%Fe-0.5wt%Mn system alloy increased from 0.3wt% to 0.4wt%, fluidity of the alloy decreased by 8.6%. When Fe content of the alloy increased from 0.15wt% to 0.6wt%, macro shrinkage ratio decreased from 6.1% to 4.1%, and micro shrinkage ratio increased from 0.04% to 0.24%. Similarly, Mn content of the alloy increased from 0.3wt% to 0.7wt%, macro shrinkage ratio decreased from 6.0% to 4.5% and micro shrinkage ratio increased from 0.12% to 0.18%. Judging from the castability of the alloy, Al-9wt%Si-0.3wt%Mg alloy with low content of Fe and Mn, 0.1wt% Fe and 0.3wt% Mn, is recommendable.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2000년도 제18회 학술발표회 논문개요집
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• pp.174-174
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• 2000

A strong antiferromagnetic coupling in Fe/Si multilayered films (MLF) had been recently discovered and much consideration has been given to whether the coupling in the Fe/Si MLF system has the same origin as the metal/metal MLF. Nevertheless, the nature of the interfacial ron silicide is still controversial. On one hand, a metal/ semiconductor structure was suggested with a narrow band-gap semiconducting $\varepsilon$-FeSi spacer that mediates the coupling. However, some features show that the nature of coupling can be well understood in terms of the conventional metal/metal multilayered system. It is well known that both magneto-optical (MO) and optical properties of a metal depend strongly on their electronic structure that is also correlated with the atomic and chemical ordering. In this study, the nature of the interfacial regions is the Fe/Si multilayers has been investigated by the experimental and computer-simulated MO and optical spectroscopies. The Fe/Si MLF were prepared by rf-sputtering onto glass substrates at room temperature with the number of repetition N=50. The thickness of Fe sublayer was fixed at 3.0nm while the Si sublayer thickness was varied from 1.0 to 2.0 nm. The topmost layer of all the Fe/Si MLF is Fe. In order to carry out the computer simulations, the information on the MO and optical parameters of the materials that may constitute a real multilayered structure should be known in advance. For this purpose, we also prepared Fe, Si, FeSi2 and FeSi samples. The structural characterization of Fe/Si MLF was performed by low- and high -angle x-ray diffraction with a Cu-K$\alpha$ radiation and by transmission electron microscopy. A bulk $\varepsilon$-FeSi was also investigated. The MO and optical properties were measured at room temperature in the 1.0-4.7 eV energy range. The theoretical simulations of MO and optical properties for the Fe/Si MLF were performed by solving exactly a multireflection problem using the scattering matrix approach assuming various stoichiometries of a nonmagnetic spacer separating the antiferromagnetically coupled Fe layers. The simulated spectra of a model structure of FeSi2 or $\varepsilon$-FeSi as the spacer turned out to fail in explaining the experimental spectra of the Fe/Si MLF in both intensity and shape. Thus, the decisive disagreement between experimental and simulated MO and optical properties ruled out the hypothesis of FeSi2 and $\varepsilon$-FeSi as the nonmagnetic spacer. By supposing the spontaneous formation of a metallic ζ-FeSi, a reasonable agreement between experimental and simulated MO and optical spectra was obtained.

• 한국표면공학회지
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• 제36권2호
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• pp.200-205
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• 2003

Thermoelectric p-type $Fe_{0.98}$ $Mn_{ 0.02}$$Si_2$ bulk specimens have been produced by mechanical alloying and consolidation by vacuum hot pressing. The subsequent isothermal annealing was not able to fully transform the mestastable as -milled powders into the $\beta$ $-FeSi_2$ phase, so that the obtained matrix consisted of not only thermoelectric semiconducting $\beta$-FeSi$_2$ but also some residual, untransformed metallic $\alpha$ $- Fe_2$$Si_{ 5}$ and $\varepsilon$-FeSi mixtures. Interestingly, $\beta$ - $FeSi_2$ was more easily obtained in the low density specimen when compared to the high density specimen. The oxidation at 700 and $800^{\circ}C$ in air led to the phase transformation of the above described iron - silicides and the formation of a thin silica surface layer.

• 한국세라믹학회지
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• 제33권1호
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• pp.74-82
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• 1996

Fe-Si based powders prepare by melting the metals in the composition of FeSi2,.Fe0.95Mn0.05Si2 and Fe0.95Co0.05Si0.2 were used as the starting materials together with a commercial FeSi2 powder to study the effect of oxidation on their thermoelectric properties. The powders were heated at 650~80$0^{\circ}C$ in dired air before forming and sintering at 1190 and 120$0^{\circ}C$ in Ar+7%H2. The microstructure and phases of the annealed specimens were observed using the optical microscopty SEM, EDS and XRD. The thermoelectric properties of the specimens were also measured. The temperature at which Seebe다 coefficient showed the maximum value increased with the degree of oxidation. Electrical conductivity showed a tendency to decrease in the oxidized samples regardless of their compositions. Seebeck coefficient of the specimen showed almost the same value even after oxidation which may be explained by the formation of the discontinuous second phases from impurities in the oxidized specimens.

• Journal of Magnetics
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• 제1권1호
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• pp.4-8
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• 1996

Employing the LMTO band method, we have studied electronic and magnetic properties of Fe/Si/Fe trilayer in which the z-direction is chosen to be (111) direction of FeSi with B2 phase, We have also determined electronic structure of bulk FeSi, as a reference material. The ground state of FeSi is paramagnetic insulator with a band gap of 0.05 eV. Band structures of Fe/Si/Fe with varying the thickness of the spacer layer reveal that the spacer layer is metallic, and the states along the growth direction do not disperse much reflecting a two-dimensional nature. Magnetic moment of Fe atom in the interfacial layer of Fe/Si/Fe is reduced a lot as compared to the bulk value, suggesting a strong hybridization between Fe and Si states. The geometry of the Fermi surface indicates that the magnetic coupling period of ~8ML (monolayers) in Fe/Si/Fe is explained with a short Fermi wave vector of bcc Si.