• 한국재료학회지
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• 제13권6호
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• pp.365-368
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• 2003

Small amounts of additives such as mol % 0.13 NiO and mol % 0.01 $CaCO_3$were added to Cu-Zn-Mg ferrites. Basic composition of the Cu-Zn-Mg ferrites was $Cu_{Cu}$X/$Fe_{0.054}$ /$Zn_{0.486}$$Mg_{0.407}$ $Fe_{1.946}$ $O_4$(group A) and $Cu_{0.263}$$Fe_{0.027}$ $Zn_{0.503}$ $Mg_{0.262}$ $Fe_{1.973}$ $O_4$(group B). Specimens were sintered at different temperatures (1010, 1030, $1050^{\circ}C$) for 2 hours in air followed by an air cooling. Then, effects of various composition and sintering temperatures on the microstructure and the magnetic properties such as inductions, coercive forces, and initial permeabilities of the Cu-Zn-Mg ferrites were investigated. The average grain size increased with the increase of sintering temperature. The magnetic properties obtained from the aforementioned Cu-Zn-Mg ferrite specimens were 1,724 gauss for the maximum induction, 1.0 oersted for the coercive force, and 802 for the initial permeability. These magnetic properties indicated that the specimens could be utilized as the core of IFT (intermediate frequency transformer) and antenna in the amplitude modulation.

• 한국세라믹학회지
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• 제33권1호
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• pp.119-125
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• 1996

Magnetic properties through controlled nucleation and crystallization wer studied for ferrimagnetic 40Fe2O3-20CaO-40SiO2 glass useful as thermoseeds for hyperthermia of tumor therapy. The maximum nucleation and crystal growth temperature are $700^{\circ}C$ and 100$0^{\circ}C$ respectively. The glass showed the maximum saturation magnetization of 168.4 emu/cm3 when nucleated $700^{\circ}C$ for 60 min and crystal grown at 100$0^{\circ}C$ for 4hrs. The maximum coercive force was 390 Oe when uncleated $700^{\circ}C$ for 60 min and crystal grown at 975$^{\circ}C$ for 2 hrs. The variation of the saturation magnetization could be well quantitatively interpreted in terms of the volume fraction of the magnetite whereas that of the coercive forces could be explained only qual.itatively in terms of the particle size of the magnetite. Hysteresis losses showed the maximum value of 0.18W/cm3 when heat treated at 100$0^{\circ}C$ for 4 hrs pre-necleated at $700^{\circ}C$ for 60 min and temperature increase of 7K under AC magnetic field of 10 kOe and 10kHz.

• 한국세라믹학회지
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• 제19권4호
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• pp.267-274
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• 1982

The sintering behavior and B-H loop properties of $Li_{0.5O4}$ with the addition of $Nb_2O_5$ and $V_2O_5$ have been investigated by observation of microstructures and measurement of semi-static hysteresis loops. The sintering temperature was lowered by the additions of $Nb_2O_5$ and $V_2O_5$ and the effect of $V_2O_5$ addition was greater than that of $Nb_2O_5$. The abnormal grain growth was observed at about 100$0^{\circ}C$(d:4.6g/㎤) and 85$0^{\circ}C$(d:4.5g/㎤) in the specimens with the addition of $Nb_2O_5$ and $V_2O_5$ respectively. The addition of $Nb_2O_5$ retulted in a large and uniform grain size, and the addition of $V_2O_5$ resulted in a uniform grain size but the final density was lower than that of the pure specimen. The squareness was increased and the coercive force was decreased by the addition of $Nb_2O_5$, and the squareness was decreased and the coercive force was increased by the addition of $V_2O_5$. These effects could be explained by a large and uniform grain size, and by a lower final density of specimens with the addition of $Nb_2O_5$ and $V_2O_5$ respectively.

• 한국세라믹학회지
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• 제16권3호
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• pp.142-154
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• 1979

The effects of microstructures and some additives $(CoO and Al_2O_3$) on the magnetic properties such as initial permeability, $\mu$-T curve, coercive force, and magnetic induction of MnZn ferrites have been studied. The powder was prepared by Hot Petroleum Drying Method. The basic composition of MnZn ferrites was 25.5mole % MnO, 22.0 mole% ZnO, 52.5 mole% $Fe_2O_3$. CoO in a concentration range from 0.05 to 0.5 mole% and $Al_2O_3$ from 2.5 to 7.5 mole% were added. Sintered density increased up to 97.5% of theoretical density. Permeability increased as average grain size increased, and that coercive force decreased as average grian size increased. Magnetic induction increased as sintered density increased. The variation of initial permeability with temperature in a temperature range from 0$^{\circ}$ to $60^{\circ}C$ was lowered (a flatter $\mu-T$ curve) as sintering temperature decreased. The compensation temperature To ofmagnetocrystalline anisotropy constant K1 and initial permeability varied with the species and amount of additives. When 0.05 mole% CoO was added to the basic composition, initial permeability at $15^{\circ}C$ increased from 5200 to 5900. The variation ofinitial permeability with temperature in a temperature range from 0^{\circ}to $60^{\circ}C$ was smaller (a flatter $\mu$-T curve) than that of the basic composition of Mn Zn ferrites. When 2.5 mole% $Al_2O_3$ was added, initial permeability at $15^{\circ}C$ decreased from 5200 to 3000. But the variation of initial permeability with temperature in a temperature range from 0$^{\circ}$to $60^{\circ}C$ was smaller (a flat ter $\mu-T$ curve) than when 0.05 mole% CoO was added. Experimental results showed that the conditions necessary for the occurrence of a very high permeability and a flat $\mu$-T curve were controversial even in a temperature range from $0^{\circ}$to $60^{\circ}C$.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.478-480
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• 2001

Fe-base amorphous films exhibit large saturation magnetostriction and soft magnetic Properties, which make them suitable for strain sensor applications. Most important material properties for the performance of these elements are the superior soft magnetic properties, such as high permeability and small coercive force, as well as magnetoelastic properties. It is well known that the strain generated in film deposition and/or post-heat treatment processes is one of important material properties, which effects on the soft magnetic properties of the film via magnetoelastic coupling. In this study, the effect of an isotropic strain in plane of magnetic films have been performed experimently. Amorphous films with the composition of (F $e_{90}$ $Co_{10}$)$_{78}$S $i_{l2}$ $B_{10}$ were employed in this study. The film with 5${\mu}{\textrm}{m}$ thick was deposed onto the polyimide substrate with 50${\mu}{\textrm}{m}$ thick by virtue of RF sputtering. The film was subject to post annealing with a static magnetic field with 500Oe magnetic field intensity at 35$0^{\circ}C$ for 1 hour. The polyimide substrate with the film was bonded with an adhesive on PZT piezoelectric substrate with 600${\mu}{\textrm}{m}$ thick in applying voltage of 500V. The change in MH loops of films due to the isotropic strain was measured by using VSM. The coercive force was evaluated from MH loops. It has shown in the results that M-H loops of films are subject to change considerably with a dc voltage, resulting of the magnetization rotation from normal to plane direction as the applied voltage is changed from 500V to 250V.50V.V.

• 한국전기전자재료학회논문지
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• 제11권6호
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• pp.486-492
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• 1998

The amorphous Co-based magnetic films have a large saturation flux density, a low coercive force, and a zero magnetostriction constant. Therefore, they have been studied for application to magnetic recoding heads and micro magnetic devices. However, it was found that the magnetic anisotropy was changed for each film fabrication processes. In this study, we investigated how to control the anisotropy of sputtered amorphous $Co_{89}Nb{8.5}Zr{2.5}$ films. After deposition, the rotational field annealing ant the uniaxial field annealing were performed under the magnetic field of 1.5 kOe. the annealing was done at the temperature range from 400 to $600^{\circ}C$ for one hour. As-deposited amorphous $Co_{89}Nb{8.5}Zr{2.5}$ thin film had saturation magnetization ($4\piM_5$) of 0.8 T, coercive force($_IH_C$) of 1.5 Oe, and anisotropy field($H_k$) of 11 Oe. The amorphous $Co_{89}Nb{8.5}Zr{2.5}$ thin films annealed by rotational field annealing at $500^{\circ}C$ for one hour was found to be isotropy, and $4\piM_5$ of 0.9 T was obtained from these films, Also, the magnetic anisotropy of as-deposited films could be controlled by uniaxial field annealing at $400^{\circ}C$ for one hour. Anisotropy field($H_k$) of 17 Oe and $4\piM_5$ of 1.0 T were obtained by this method.

• 한국자기학회지
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• 제12권4호
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• pp.154-159
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• 2002

벌크 비정질 형성능과 큰 포화자속밀도를 가지는 FeBSiNb계 아몰퍼스 합금 리본을 22~102$\mu\textrm{m}$의 두께 범위에서 단롤형 액체 급냉법으로 제조하였다. 이 합금은 두께 증가에 따라 보자력이 감소하고 최대투자율 및 교류투자율이 증가하였으며, 자기이력곡선의 각형비가 감소하였다. 한편 전기 비저항은 두께와 상관없이 거의 일정한 값을 나타내었다. 또 지구 관찰 결과, 두께가 증가하면 내부 자기 이방성의 변화에 따라 자구가 미세화 되고 보다 복잡한 자구 구조를 갖는 것으로 나타났다. 두께 81$\mu\textrm{m}$인 합금의 경우, 24 mOe의 작은 보자력과 1KHz에서 12,000이상의 높은 실효투자율을 나타내어 일반적인 고 연자성 비정질 합금(두께 약 20$\mu\textrm{m}$)의 특성을 능가하였다. 이와 같은 두꺼운 FeBSiNb 비정질 합금의 우수한 연자성은 자벽이동에 대한 표면 고착 효과의 감소 및 수직자기이방성 성분의 출현과 미세화 된 자구 구조에 그 원인이 있는 것으로 평가되었다.

• 한국진공학회지
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• 제9권4호
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• pp.389-393
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• 2000

Metalloid의 양이 거의 일정(B, Si 각각 l0 at.% 정도)하게 유지되는 상황에서 FeCoSiB 박막내의 Co함량 증가가 여러 가지 자기적 특성에 미치는 효과, 그리고 열처리 온도와 시간에 따른 막의 자성특성 변화를 관찰해 보았다. dc magnetron sputter를 이용하여 비정질 합금 자성박막을 증착하였으며, 비정질의 막을 형성하기 위하여 기판은 수냉하였다. 막의 조성은 순철 target위에 올려놓는 pellet의 수를 조절하여, 대략 $Fe_{80-X}Co_XBi_{10}Si_{10}$ (X=8~18 at.%)로 하였으며, 증착된 막의 조성은 ICP 분석법을 이용하여 조사하였다. Sputtering에 의해 증착된 박막의 결정화 유무는 XRD로 분석하였으며, 보자력과 포화 자화값 등의 자기적 성질은 VSM을 이용하여 측정하였다. 실험결과에 따르면 막내 Co 함량이 증가함에 따라 보자력은 감소하는 경향을 나타내었으며, 포화자화 값은 Co 함량이 대략 10 at.%에 도달할 때까지는 증가하다가 그 이상에서는 감소하는 현상을 나타내었다. 그리고 증착 과정중에 막에 생기는 잔류응력의 제거효과를 관찰하기 위해 열처리 온도(100, 200, $300^{\circ}C$)와 시간(0~60분)을 변화시키며 실험한 결과, 예상되었던 바대로 잔류응력의 감소로 인해 Co 첨가시와 마찬가지로 보자력이 감소하는 결과를 나타내었다.

• 한국자기학회지
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• 제5권1호
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• pp.1-7
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• 1995

급속응고법중 단롤법을 이용하여 Fe-B계에 Co 및 Nb과 Al이 치환된 (Fe/sub 0.85/Co/sub 0.15/)/sub 75/ Al/sub 7/B/sub 18-x/Nb/sub x/(x = 2, 4, 6)와 (Fe/sub 0.85/Co/sub 0.15/)/sub 75/Al/sub y/B/sub 21-y/Nb/sub 4/ (y = 3, 5, 7, 9)합금을 급속응고장치로 단롤법을 이용하여 리본상으로 제작한후, 이들 합금의 초미세결정립 제조 가 능성과 자기적 특성의 조성 및 온도 의존성을 조사하였다. 초미세결정립합금은 y = 9를 제외한 전조성에서 제조가 가 능하였다. 포화자화 값은 열처리 후 증가하였고 Nb 함량이 증가하면 감소하였으며 상대적으로 Al과 B의 영향은 적었 다. 50 kHz에서 조사한 초투자율은 초미세결정립이 형성된 후가 열처리 전보다 2배이상 증가하였으며, 항자력과 교류 자기이력손실은 반대로 1/2이하로 감소하였다.

• 한국자기학회지
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• 제18권1호
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• pp.9-13
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• 2008

에어로졸 성막법으로 제작된 Bi:YIG($Bi_{0.5}Y_{2.5}Fe_5O_{12}$) 막에 있어서, 에어로졸 입사각도가 광학적 특성과 자기적 특정에 미치는 영향에 대하여 조사하였다. 에어로졸입사각도를 0도에서 30도로 증가시킴으로써 입사광의 파장이 450 nm일 때 광투과율은 약 80%의 향상이 얻어졌다. 그 이유는 에어로졸 입사각도를 높임으로써 입자간 응집체 등에 의해서 생성되는 막표면 혹은 막내부의 결함을 줄일 수 있기 때문으로 고찰되었다. 또한, 에어로졸 입사각도를 높임으로써 Bi:YIG막의 보자력을 크게 줄일 수 있다는 것을 실험적으로 검증할 수 있었다. 그 이유로는 에어로졸 입사각도를 높임으로써 입자와 기판간의 충돌에너지의 변화와 자벽이동의 방해가 되는 결함의 감소가 정성적으로 예상되었다.