• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제49권2호
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• pp.98-102
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• 2000

Ferroelectric PZT heterolayered thin films were fabricated by spin coating method on the Pt/Ti/SiO2/Si substrate using PZT(10/90) and PZT(90/10) m7etal alkoxide solutions. All PZT heterolayered films showed a homogeneous grain structures without presence of rosette structure. It can be assumed that the lower PZT layers played a role of nucleation site for the formation of the upper PZT layer. Pb-deficient PZT phase was formed at PZT/Pt interface due to the diffusion of Pb element into a Pt bottom electrode. The relative dielectric constant and the dielectric loss of the PZT-6 film were 567 and 3.6%, respectively. Increasing the number of coatings, remanent polarization and coercive field were decreased and the values of the PZT-6 heterolayered film were $7.18\muC/cm^2$ and 68.5kV/cm, respectively. Leakage current densities were increased with increasing the number of coatings, and the value of the PZT-4 film was about $7\times10-8A/cm^2$ at 0.05MV/cm.

• 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.

• Journal of Magnetics
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• 제18권3호
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• pp.235-239
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• 2013

The effect of Dy addition on the microstructure and magnetic properties of the sintered NdFeB magnets was investigated. The results of the microstructure analysis showed that Dy-free and Dy-doped samples are composed of $Nd_2Fe_{14}B$ (P42/mnm) and a trace of Nd-rich phase. Dy addition reduces significantly the pole density factor of (004), (006) and (008) crystal faces as estimated by the Horta formula. Accordingly, the coercivity of the Dy-doped sample increases from 2038 $kA{\cdot}m^{-1}$ up to 2288 $kA{\cdot}m^{-1}$. The $H_{cj}(T)/M_s(T)$ versus $H^{min}_N/M_s(T)$ (Kronm$\ddot{u}$ller-plot) behavior shows that the nucleation is the dominating mechanism for the magnetization reversal in these two kinds of magnets, and two microstructural parameters of ${\alpha}_k$ and $N_{eff}$ are obtained. The Kronm$\ddot{u}$ller-Plot gives evidence for an increase of the ${\alpha}_k$ responsible for an increase of the coercivity as the result of the increase of the magnetic field as the magnetic domain reversed.

• 한국자기학회지
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• 제12권3호
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• pp.94-98
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• 2002

20nm이하의 얇은 박막에서도 높은 보자력이 요구되는 Ti/CoCrPt 수직자기기록박막의 보자력 향상을 위해 Al, Cu, Ni, Cr, Ag, Mg, Fe, Co, Pd, Au, Pt, Mo, Hf등의 여러 하지층과 제조조건이 보자력에 미치는 영향을 조사하였다 이들 중 Ag과 Mg하지층은 Ti/CoCrPt박막의 보자력을 향상시켰으며 특히 2nm Ag 하지층을 사용할 경우 10nm CoCrPt 박막에서 2200 Oe의 높은 보자력을 보일뿐 아니라 $\alpha$값을 낮추는 효과가 있었다. 그러나 Ag를 하지층으로 사용하면 기대와는 달리 Ti(002)면의 우선배향 성장이 전혀 일어나지 않아 보자력 증대에 다른 기구가 작용하는 것으로 판단되었다. 그리고 표면의 거칠기가 큰 기판에서는 보자력뿐만 아니라 역자구생성자계도 감소하였다.

• Journal of Magnetics
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• 제14권1호
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• pp.36-41
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• 2009

Magneto-optical Kerr effect (MOKE) magnetometry was used to investigate magnetization reversal dynamics in 30-nm NiFe/15-nm FeMn, 15-nm FeMn/30-nm CoFe bilayers, and 30-nm NiFe/(2,10)-nm FeMn/30-nm CoFe trilayers. The in-plane magnetization components of each ferromagnetic layer, both parallel and perpendicular to the applied field, were separately determined by measuring the longitudinal and transverse MOKE hysteresis loops from both the front and back sides of the film for an oblique incident s-polarized beam. The magnetization of the FeMn/CoFe bilayer was reversed abruptly and symmetrically through nucleation and domain wall propagation, while that of the NiFe/FeMn bilayer was reversed asymmetrically with a dominant rotation. In the NiFe/FeMn/CoFe trilayers, the magnetic reversal of the two ferromagnetic layers proceeded via nucleation and domain wall propagation for 2-nm FeMn, but via asymmetric rotation for 10-nm FeMn. The exchange-biased ferromagnetic layers showed the magnetization reversal along the same path in the film plane for the decreasing and increasing field branches from transverse MOKE hysteresis loops, which can be qualitatively explained by the theoretical model of the exchange-biased ferromagnetic/antiferromagnetic systems.

• 대한기계학회논문집B
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• 제21권12호
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• pp.1563-1575
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• 1997

To understand EHD nucleate boiling heat transfer enhancement, EHD effects on R-113 nucleate boiling heat transfer in a non-uniform electric field were investigated. The pool boiling heat transfer and the dynamic behavior of bubbles in d.c./a.c. electric fields under a saturated or subcooled boiling were studied by using a plate-wire electrode and a high speed camera. From the pool boiling heat transfer study, the shift of the pool boiling curve, the increase of the heat transfer and the delay of ONB and CHF points to higher heat fluxes were observed. From the dynamic behavior of bubbles, it was observed that bubbles departed away from the whole surface of the heated wire in radial direction due to EHD effects by a nonuniform electric field. With increasing applied voltages, the bubble size decreased and the active nucleation site and the departure number of bubbles showed the different trend. The present study indicates that the EHD nucleate boiling heat transfer is closely connection with the dynamic behavior of bubbles and the secondary flow induced near the heated surface. Therefore, the basic studies on the bubble behavior such as bubble frequency, bubble diameter, bubble velocity and flow characteristics are necessary for complete understanding of the enhancement mechanism of the boiling heat transfer using an electric field.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2009년도 제40회 하계학술대회
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• pp.1447_1448
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• 2009

In this paper, each specimen blended at weight proportions of 80% HDPE to 20% EVA, 70% HDPE to 30% EVA, 60% HDPE to 40% EVA, and 50% HDPE to 50% EVA was manufactured respectively. The insulation performances of the proposed insulator were compared with conventional XLPE, main insulating material of CV cable on the basis of the investigation results of DC insulation performances. From the space charge density, electric field and potential profiles with raising DC voltage and time variation in HE82, distortion of electric field distribution was improved. As EVA mixed into the bulks acts as nucleation in crystallization process of HDPE, the size of spherulites became decreased and finally formed continuous network structure. Ultimately it resulted from extinction of space charge in the interfacial region of spherulites.

• 공업화학
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• 제34권2호
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• pp.111-120
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• 2023

이산화탄소 순환 물질 중 대표적인 광물인 탄산칼슘의 형성 과정을 관찰하고, 대표적 조절 변수인 마그네슘-칼슘 이온의 혼합 비율(Mg/Ca 비)과 온도가 pre-nucleation cluster (PNC) 및 탄산칼슘 형성에 미치는 영향을 분석하고자 실험과정에서 칼슘 이온 선택성 전극(calcium ion selective electrode, Ca ISE)을 이용하여 핵형성 과정을 연구하였다. 실험결과 미량의 결정이 형성되었으며 표면 원소 분석을 위해 에너지 분산 X선 분석법(energy dispersive X-ray spectroscopy, EDS)을 사용하였고, 형상 분석을 위해 주사 전자 현미경(field emission scanning electron microscope, FE-SEM)을 사용하였다. Mg/Ca 비와 온도 조건에 따라 다양한 형상의 결정질 탄산칼슘(방해석, 아라고나이트 등)을 확인하였으며 Ca ISE로부터 얻은 칼슘 이온 농도 그래프는 탄산칼슘 형성 과정을 보여주었다. 칼슘 이온 농도 그래프 분석을 통해 마그네슘 이온은 칼슘 이온과 탄산 이온의 결합을 방해하고 PNC 간 응집을 지연시켜 핵형성 및 탄산칼슘의 형성을 지연시킴을 확인하였다. 반면 온도는 이와 반대되는 효과를 보였으며, 본 실험 조건에서는 마그네슘 이온보다 더 큰 영향을 미쳤다. 또한 Mg/Ca 비와 온도에 따라 탄산칼슘의 형상이 뚜렷하게 변화하여 두 인자는 탄산칼슘 형성 과정에 전반적으로 영향을 미치는 중요 조절 변수임을 확인하였다.

• 한국자기학회지
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• 제15권2호
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• pp.72-75
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• 2005

변압기 철심으로 널리 사용되고 있는 $3.2{\%}$ Si-Fe 방향성전기강판에서 인장응력을 인가하면서 자기이력과정 동안 교류 섭동 자기장의 2차 고조파 파형을 관측하였다. 관측된 파형을 인가 자기장에 의한 자구 재배열과정에서 일어나는 비선형, 비대칭 자기유도에 의해 분석하였다. 인장응력 하에서 구한 2차 고조파 파형은 자구 생성 및 소멸 자기장에서 피크를 갖는데, 인장응력의 크기에 따라 피크간격은 선형적으로 감소하며, 그 기울기를 이용하여 포화자기변형을 측정할 수 있는 방법을 제시한다.

• Journal of Magnetics
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• 제16권2호
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• pp.83-87
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• 2011

The vortex-driven magnetization process of micron-sized, exchange-coupled square elements with composition of $Ni_{80}Fe_{20}$ (12 nm)/$Ir_{20}Mn_{80}$ (5 nm) is investigated. The exchange-bias is introduced by field-cooling through the blocking temperature (TB) of the system, whereby Landau-shaped vortex states of the $Ni_{80}Fe_{20}$ layer are imprinted into the $Ir_{20}Mn_{80}$. In the case of zero-field cooling, the exchange-coupling at the ferromagnetic/antiferromagnetic interface significantly enhances the vortex stability by increasing the nucleation and annihilation fields, while reducing coercivity and remanence. For the field-cooled elements, the hysteresis loops are shifted along the cooling field axis. The loop shift is attributed to the imprinting of displaced vortex state of $Ni_{80}Fe_{20}$ into $Ir_{20}Mn_{80}$, which leads to asymmetric effective local pinning fields at the interface. The asymmetry of the hysteresis loop and the strength of the exchange-bias field can be tuned by varying the strength of cooling field. Micromagnetic modeling reproduces the experimentally observed vortex-driven magnetization process if the local pinning fields induced by exchange-coupling of the ferromagnetic and antiferromagnetic layers are taken into account.