• 한국세라믹학회지
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• 제29권5호
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• pp.383-390
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• 1992

We investigated the effect of substrate on the properties of the Ni-Zn-Cu ferrite thin films deposited on SiO2 (1000∼3000${\AA}$) / Si (100) substrate at various conditions by rf magnetron sputtering. A disktype Ni-Zn-Cu ferrite sintered by conventional ceramic process and argon gas were used as a target and a sputtering gas, repectively. The compositions of the thin films measured by EPMA were similar to target composition (Fe: 65.8 at%, Ni: 12.7 at%, Cu: 6.7 at%, Zn: 14.8 at%) irrespective of substrate temperature. Amorphous thin films were deposited when substrate was not intentionally heated, but the films came to crystallize with increasing substrate temperature, and crystalline thin films were deposited at substrate temperature above 200$^{\circ}C$. Below 250$^{\circ}C$ saturation magnetization (Ms), remanence (Mr) and coercivity (Hc) of the ferrite thin film increased with the substrate temperature due to the increase of grain size and the improvement of crystallinity. And above 250$^{\circ}C$, Ms, Mr increased slightly, but Hc of the amorphous thin films increased due to crystallization, whereas that of the crystalline thin films decreased because of grain growth and stress release.

• 한국분말재료학회지
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• 제18권1호
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• pp.24-28
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• 2011

Effect of Cu content on microstructural and magnetic properties of a $(Nd_{26.06},Dy_{6.51})Fe_{bal.}$ $Cu_xB_{0.97}$(wt.%), (x = 0.2, 0.3, 0.4, 0.5) strip-cast was studied. The average inter-lamellar spacing in the free surface and wheel side of the strip cast increased as the Cu content increases. The grain uniformity, the grain alignment, and (00L) texture of the strip cast increased with Cu contents up to 0.4 wt.%. These microstructural changes were attributed to the decrease of the effective cooling rate of the melted alloy caused by the decrease of the melting temperature of resulting from Cu addition. Coercivity and remanence were increased because of the grain alignment and (00L) texture improvement with Cu contents up to 0.4 wt.%.

• Journal of Magnetics
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• 제1권2호
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• pp.75-81
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• 1996

Study on the HDDr Characteristics of Nd16Fe76-xB8Zrx (x=0-2.0) Alloys and the Magnetic Properties of the HDDR Materials Nd16Fe76-xB8Zrx (where x=0-2.0) have been studied to see the effect of Zr addition on HDDR characteristics. A particular emphasis was place upon the anisotropy of the HDDR material. Anisotropy of the HDDR powder material has been evaluated by comparing the remanence values of the aligned sample measured along the aligning direction and the direction perpendicular to it. The HDDR characteristics of the alloys were investigated by means of DAT and TPA. Magnetic chracterisation of the HDDR processed materials was performed using a VSM and a TMA. The magnetic domain structure of the HDDR materials was examined by means of polarised microscope using a solid HDDR processed material. It has veen found that small addition (0.1 at %) of Zr to Nd-Fe-B-type alloy retards thedisproportionatio kinetics of the hydrogenated material. Desorption characteristic of the disproportionated materials has been found not to be affected significantly by the Zr addition. The Zr addition has been found to facilitate size of the powder. As the particle size decreases, the intrinsic coercivity decreases radically, and this is explained in terms of structural damage and/or oxidation caused during mechanical milling. It has also been found that the degree of alignment representing the anisotropic character of the HDDR powder is enhanced with decreasing particle size. Alloys with compositions based on

• Journal of Magnetics
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• 제9권2호
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• pp.40-46
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• 2004

The magnetic properties of sputtered ($Ni_{83}Fe_{17}/Au/Co/Au$) multilayers with various thicknesses of Au (0.5 {\leq} t_{Au} {\leq} 3 nm), Ni-Fe ($1{\leq}t_{Ni-Fe}{\leq}4nm$) and Co ($0.2{\leq}t_{co}{\leq}1.5nm$) layers were characterized. An alternating in-plane and out-of-plane anisotropy of the ferromagnetic layers was achieved for the structures ($t_{Au}{\geq}1.5nm$) showing a weak coupling between the Ni-Fe layers with an in-plane anisotropy and the Co layers ($0.3{\leq}t_Co{\leq}1.2nm$) with a perpendicular anisotropy. For such a structure, a detailed discussion on the GMR effect is presented, relating to the magnetization reversal from a mutually perpendicular magnetic configuration at the remanence to a parallel one at the saturation. An influence of the dense labyrinth domain structure on the magnetoresistance effect is also addressed.

• Journal of Magnetics
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• 제19권3호
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• pp.205-209
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• 2014

$MnBi_{1-x}Ti_x$ (x = 0, 0.4, 0.7, 1) alloys were prepared by arc-melting, followed by heat treatment. X-ray diffraction (XRD) and vibrating sample magnetometer (VSM) were used to measure and investigate the phase structure and magnetic properties. The temperature dependent magnetization curves indicate that the phase transitions between LTP and HTP MnBi occur with heating or cooling in $MnBi_{1-x}Ti_x$ ($x{\leq}0.7$) samples. However, MnTi samples are in $Mn_2Ti$ single-phase, with very low magnetic properties. Furthermore, the coercivity exhibits a positive temperature coefficient. The results show that the optimal content of Ti for the coercivity of $MnBi_{1-x}Ti_x$ alloy is x = 0.4. For MnBi sample, the coercivity reaches a maximum value of 1.13 T at 550 K. However, the remanence and energy product show apparent decrease with the addition of Ti in $MnBi_{1-x}Ti_x$ alloys.

• 한국표면공학회지
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• 제29권6호
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• pp.839-846
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• 1996

Epitaxial (La, Sr)$CoO_3/Pb(Zr,\;Ti)O_3/(La,\;Sr)CoO_3$by pulsed laser deposition for ferroelectric field effect transistor. Epitaxial $LaCoO_3/Pb(Zr,\;Ti)O_3/(La,\;Sr)CoO_3$ heterostructures exhibited 70$\mu C/cm^2$ and 17 $\mu C/cm^2$at a positively and negatively poled states, respectively. On the other hand, epitaxial (La, Sr)$CoO_3/Pb(Zr,\;Ti)O_3/LaCoO_3$heterostructures show the remnant polarization states opposite to the $LaCoO_3/Pb(Zr,\;Ti)O_3/(La,\;Sr)CoO_3$ heterostructures. This indicates that the interface between (La, Sr)$CoO_3$ (LSCO) and $Pb(Zr, Ti)O_3(PZT)$ layers affects the asymmetric polarization remanence through electrochemical nature. The resistivity of $LaCoO_3$ (LCO) layer was found to be dependent on an ambient oxygen, primarily the ambient oxygen pressure during deposition. The resistivity of the LCO layer varied in the range of 0.1-100 $\Omega$cm. It is suggested that, with an appropriate resistivity of the LCO layer, the LCO/PZT/LSCO heterostructure can be used as the ferroelectric field effect transistor.

• 한국분말재료학회지
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• 제17권5호
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• pp.359-364
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• 2010

In an attempt to optimize the magnetic properties of (Nd, Dy)-Fe-B sintered magnets, hydrogenation and post-sintering heat treatment processes were investigated at various hydrogenation temperatures and heat treatment temperatures. The coercivity of (Nd, Dy)-Fe-B sintered magnets hydrogenated at $400^{\circ}C$ increased to about 1.2 kOe without any detrimental effect on the remanence. Moreover, the coercivity of the magnets was enhanced further by a consecutive $2^{nd}$ and $3^{rd}$ step heat treatment. These results eventually leaded to the reduction of the Dy content in a high coercive (> 30 kOe) (Nd, Dy)-Fe-B sintered magnets, as much as 10%.

• 한국자기학회지
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• 제6권5호
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• pp.310-316
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• 1996

본 연구에서 인가 자장의 세기, 압출 금형의 온도 및 압출 속도가 페라이트계 이방성 압출 본드 자석의 자기적 특성에 미치는 영향을 조사하였다. 압출 본드 자석 단면에 대한 X-선 회절실험 결과 압출 금형 내의 용융 흐름에 의해 자성 분말의 자장 방향으로의 배향이 억제됨을 알 수 있었다. 압출 금형의 온도가 $20^{\circ}C$ 일 때 4 kOe의 인가자장에서 82 %의 배향도를 얻을 수 있었으며, Sr-페라이트 분말의 충전율이 50 vol%일 때 잔류자속밀도 2.2 kG인 압출 본드 자석을 제조할 수 있었다.

• 한국자기학회지
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• 제6권5호
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• pp.334-339
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• 1996

도포형 자기기록매체에 있어서 자성분의 size와 특성이 자기기록 특성에 미치는 영향을 조사하기위하여 size가 다른 각각의 자성분으로 만든 도료를 이용하여 자기 tape를 제조하고 자성분의 분산성 및 전자 변환 특성을 측정하였다. 자성분의 분산성은 입자 size의 영향보다 입자의 형태 및 자성분의 표면화학특성에 크게 의존하며 자성분의 입자 size가 작아질 수록 자성분의 충진성은 향상 되고 tape의 remanence 특성과 출력 특성 및 noise 특성이 향상되어 고출력, 저 noise의 넓은 dynamic range의 출력이 나타남을 확인하였다. 따라서 고출력의 자기 tape를 제조하기 위하여는 자성분의 size, 형상, 표면화학 특성 및 자기특성이 자성분 선정의 중요한 요건임을 확인하였다.

• 한국자기학회지
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• 제14권3호
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• pp.105-108
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• 2004

나노크기의 기공을 갖는 AAO(Anodic Aluminum Oxide)를 이용하여 Si 기판 위에 열 증착 방식으로 Ni 나노구조체를 제작하였다. 제작된 나노구조체는 직경과 높이가 80nm정도로 거의 비슷한 원기둥 형태를 보였다. Ni 나노구조체의 자기적 특성은 광자기효과(Magneto-Optic Kerr effect)를 이용하여 측정하였고, 함께 성장시킨 박막(continuous film)과 비교하였다. 종횡비(aspect ratio)가 1 : 1 정도인 나노구조체의 자화용이축은 평면방향으로 자화용이축을 보이는 박막과는 달리 수직자기이방성을 보여주었으며, 수직 및 수평방향으로 자기장을 가하면서 얻은 자기이력곡선(hysteresis loop)으로부터 나노구조체의 포화자기장(saturation field)과 보자력(coercivity)이 박막과는 많은 차이를 보였다. 박막에서 거의 무시할 만한 값을 갖는 수직방향의 자기이력곡선에서 측정된 잔류자화(remanent magnetization) 나노구조체에서는 0.3으로 크게 증가했다.