• Journal of the Korean Magnetics Society
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• v.2 no.2
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• pp.114-118
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• 1992

아크로를 이용하여 제작한 NdF $e_{12-x}$ $Ti_{x}$ (1 .leq. x .leq. 2) 합금의 상분석 결과 이들 합금은 ThM $n_{12}$ 구조의 경자성상(1-12상) 과 반강자성의 F $e_{2}$Ti 및 연자성의 .alpha. -Fe 등으로 구성되며, x=1.3 인 NdF $e_{10.7}$ $Ti_{1.3}$ 조성에서 단상에 가까운 ThM $n_{2}$ 구조가 얻어짐이 밝혀졌다. 한편, 합금중의 1-12 상은 50 .mu. m - 100 .mu. m 의 사각주 형태로 생성되며, FeTi은 1-12상의 결정립계에 고립된 입자의 형태로 존재한다. NdF $e_{10.7}$ $Ti_{1.3}$ 합금을 질화처리할 경우 단위포의 체적, 자화, 이방성자장 및 큐리온도가 증가하며, 이합금을 500 .deg. C 에서 15분간 질화처리한 NdF $e_{10.7}$ $Ti_{1.3}$ $N_{x}$ 의 비포화자화, 이방성자장 및 큐리온 도는 각각, .sigma. $_{s}$ =128 A $m^{2}$/kg $H_{A}$=6400 kA/m (80 kOe) 및 Tc=470 .deg. C로 질화처리 전에 비하여 크게 증가한다.크게 증가한다. 증가한다.

• Journal of the Korean Magnetics Society
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• v.15 no.1
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• pp.25-29
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• 2005

Magnetic properties of YIG films grown by solid phase epitaxy (SPE) was measured as a function of temperature with focus on magneto-crystalline and perpendicular magnetic anisotropy. Perpendicular magnetic anisotropy was not induced in the SPE YIG films annealed at low temperature by relaxing residual stress through formation of dislocation. On the contrary the films annealed at high temperature showed perpendicular magnetic anisotropy which shows very low density of dislocation. Perpendicular magnetic anisotropy field decreased linearly up to a high temperature of $230^{\circ}C$ above which magneto-crystalline anisotropy disappeared. Coercivity also decreased linearly with temperature up 세 $230^{\circ}C$. Magneto-crystalline anisotropy of perpendicular anisotropy induced epitaxial (111) YIG films can be measured using $H_k=4K_1/3M_s$. Temperature behavior of initial susceptibility can be successfully explained by Hopkinson effects. Curie temperature of YIG films grown on GGG substrate with high paramagnetic susceptibility can be easily measured using the results.

• Korean Journal of Materials Research
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• v.7 no.9
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• pp.728-732
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• 1997

비정질 금속 $Co_{66}$F $e_{4}$Ni $B_{14}$S $i_{15}$ 의 표면층 제거에 대한 자기임피턴스 효과는 시료의 길이방향에 평행한 일축자기장에 대하여 측정하였다. MIR(Magnetoimpedance Ratios)은 비정질 금속의 두께가 얇아짐에 따라 감소하고, 전류에 비례하여 증가하는 경향을 나타내었다. 인가전류 주파수에 대한 MIR과 자기장의 감도는 모든 시료에서 주파수에 비례하여 증가하며 수 MHz 부근에서 최대값을 가지고 점차 감소하는 경향을 나타내었다. 시료의 표면층제거에 기인한 이방성자기장의 변화는 MI $R_{Max}$을 나타내는 외부 자기장을 감소시키지만, MIR은 표면층 제거에 따른 부피효과에 기인하여 감소하였다....

• Journal of the Korean Magnetics Society
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• v.3 no.3
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• pp.196-200
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• 1993

$(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ compounds have tetragonal $ThMn_{12}$-type structure and show the uniaxial magnetocrystalline anisotropy with the easy magnetization c-axis. Among the $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ series, RE=Sm shows the highest anisotropy field of 11200 kA/m(140 kOe). On the other hand, RE=Nd has the highest saturation magnetization of $122.3\;Am^{2}/kg$(122.3 emu/g) and RE=Gd the highest Curie temperature of $326^{\circ}C$.

• Resources Recycling
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• v.11 no.5
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• pp.16-20
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• 2002

This experiment was carried out to examine the effects of La-Co substitution on Sr-ferrite. The magnetic properties of calcined and sintered materials varied with the substitutional amount of La and Co elements in Sr-ferrite. Anisotropy field and coercivity for Sr ferrite were increased with raising La-Co substitution amounts. The microstructure observation for Sr ferrite substituted by La-Co revealed that La-Co inhabited grain growth during calcination and promoted lateral grain growth during sintering. The relationship between $B_{r}$ and $_{i}$ /$H_{c}$ for La-Co substituted Sr-ferrite was found to be $B_{r}$$≒0.097_{i}$ /$H_{c}$/+4500. In case of $SrFe_{12}$ $O_{19}$, $B_{r} was 4090 G and $_{ i}$$H_{c}$ was 3560 Oe, but $B_{r}$ was 4080 G and and $_{i}$ $H_{c}$ was 4800 Oe for $Sr_{0.7}$ $La_{0.3}$ $Fe_{11.7}$ /$Co_{0.3}$ $O_{19}$.

• Electrical & Electronic Materials
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• v.8 no.6
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• pp.811-815
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• 1995

회토류계 영구자석은 종래의 Ferrite계나 Alnico계와 비교해서 대단히 강하여, 전기전자부품의 소형화에 크게 기여하고 있다. 최근에는, 전자기기산업 이외의 분야에 있어서도 그의 응용이 확대되어가고 있는 추세로 자성재료의 생산액은 매년 증가하고 있다. 회토류계 영구자석재료의 연구는 1960년대에 시작되어 Sm $Co_{5}$, Sm$_{2}$ $Co_{17}$ 화합물의 등장을 거쳐 현재는 1982년데 Sagawa 및 Croat가 독자적으로 발견한 Nd$_{2}$ Fe$_{14}$B 자석이 주류로 되고 있다. 그렇지만 이 화합물에는 다른 영구자석에 비하여 큐리온도가 낮은 결점이 있어서, 아직도 새로운 화합물의 탐색이 계속되고 있다. 그 중에서도, 1990년대에 Coey에 의해서 최초로 학회지에 보고되어진 Sm$_{2}$Fe$_{17}$N$_{x}$는, Nd$_{2}$Fe$_{14}$B와 같은 정도의 이론 최대에너지급, Sm $Co_{5}$에 대등한 거대한 이방성자장, 750K에 달하는 큐리온도등의 우수한 성질을 갖고 있어 Nd$_{2}$Fe$_{14}$B를 극복하는 자성재료로서 큰 기대가 되어진다. 되어진다.진다.

• Journal of the Korean Magnetics Society
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• v.5 no.5
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• pp.858-863
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• 1995

The nitrogenation process and magnetic properties of $Sm_{2}Fe_{17}N_{x}\;(0{\leq}x{\leq}3)$ were investigated. During the initial nitrogenation process, the nitrogen content had linear relation with the square root of nitrogenation time, and the activation energy for the process was calculated to be 102.4 kJ/mol. The magnetic properties of $Sm_{2}Fe_{17}N_{x}$ were strongly dependent on the nitrogen content and the composition having $Sm_{2}Fe_{17}N_{2.8}$ showed optimum magnetic properties with a Curie temperature of 450 oC. The intrinsic magnetic properties of the nitride at room temperature were $M_{s}=1147\;emu/cm^{3},\;K_{1}=4.6{\times}10^{7}erg/cm^{3},\;K_{2}=6.0{\times}10^{7}erg/cm^{3}\;and\;H_{A}=290\;kOe$, respectively.

• Journal of the Korean Magnetics Society
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• v.2 no.3
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• pp.239-243
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• 1992

It has been found that B is very effective for the increase of magnetization and Curie temperature in $NdFe_{11}TiN_x$-type compounds having $ThMN_{12}$-type structure. Experimental results have shown that magnetization and Curie temperature of $NdFe_{10.7}TiB_{0.3}N_x$ are 148 $Am^2$/kg and $560^{\circ}C,$ respectively, by about 20 $Am^2$/kg and $90^{\circ}C$ higher than those of $NdFe_{10.7}Ti_{1.3}N_x.$ On the other hand, Mo is effective for the increase of anisotropy field, and it seems to strongly inhibit the formation of ${\alpha}-Fe$ phase during the nitrification treatement. The anisotropy field of $NdFe_{10.7}TiMo_{0.3}N_x$ is about 7960 kA/m (100 kOe) which is about 1590 kA/m (20 kOe) higher than that of $NdFe_{10.7}Ti_{1.3}N_x$.

• Journal of the Korean Magnetics Society
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• v.20 no.6
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• pp.228-233
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• 2010

The microwave permeability was measured in order to analyze the thickness dependence of loss properties in CoFeHfO thin films with varying thickness of t = 57~1368 nm. A single resonance peak (P1) at 2.95 GHz was appeared in the samples with thickness less than 405 nm, while second resonance peak (P2) at 547MHz was additionally appeared in the samples with thickness greater than 405 nm. The P2 was originated by the angle distribution of the easy axis, which was confirmed from the measured results of the change of imaginary permeability with applied magnetic field in the sample of 1368 nm thickness and low field torque curves. If the second peaks can be reduced by minimizing the angle distribution of the easy axis, the CoFeHfO thin films with thickness greater than 400 nm can be used for the compact microwave devices operated at up to 2 GHz ranges.