• Journal of Magnetics
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• 제8권4호
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• pp.164-168
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• 2003

In high density recording system, the recording head field on a medium should be focused in small bit area and should have a sufficient value to overcome the medium coercivity, which resulted in head saturation. In this paper, an efficient method to access the head field and field gradient considering head saturation is presented. The magnetic vector potential on the head surface is pre-calculated considering head saturation in several cases and accumulated into database. The head field on the recording media is easily produced solving Laplace equation using accessed magnetic vector potential boundaries. The computed head field is compared with a quantified magnetic force microscopy measurement.

• 한국진공학회지
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• 제4권S2호
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• pp.24-29
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• 1995

The magnetic amd magneto-optical(MO)properties of Co-based multilayered(ML)films are known to vary sensitively according to the manufacturing methods and the film microstructures. Co/Pd and Co/Pt ML films with ultrathin layers of Co were prepared by alternating deposition in an ultrahigh-vacuum physical-vapor-deposition system. The individual layer thicknesses of the samples were estimated making use of the angular positions of x-ray diffraction peaks. The magnetic and MO properties were investigated, and correlated systematically to the structural parameters of the films. A Kerr spectrometer was self-manufactured to measure the MO properties such as Kerr rotation angle, ellipticity and reflectivity. The rms surface roughness was also measured using atomic force microscopy. Some of the samples showed good properties for MO medium, such as large perpendicular magnetic anisotropy and Kerr rotation, and perfect squareness of the magnetic hysteresis loop.

• 한국재료학회지
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• 제12권10호
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• pp.791-795
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• 2002

We studied the physical properties of $Co_3$$O_4$-added Ni-Zn ferrite which were sintered at 1050~110$0^{\circ}C$ for 2 hours. X-ray diffraction showed a spinel structure, and optical microscopy showed grain sizes of 5 to 10 $\mu\textrm{m}$. As the sintering temperature was increased from $1050^{\circ}C$ to $1070^{\circ}C$, the initial permeability and magnetic induction increased, and both of the loss factor and the coercive force decreased. The Curie temperatures were about $^234~245{\circ}C$ with added $Co_3$$O_4$. The initial permeability was 350 to 420 and maximum magnetic induction density and coercive force 4870G to 4980G and 0.15 Oe to 0.21 Oe, respectively which were similar to those of Ni-Zn ferrite synthesized in the conventional process. The frequency of specimen was in the range of 1MHz to 300MHz. In the plot of initial permeability vs. frequencies, a $180^{\circ}C$ rotation of the magnetic domain could be perceived in a broad band of microwave before and after the resonance frequency.

• Journal of Magnetics
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• 제13권4호
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• pp.163-166
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• 2008

Multiferroic $CoCr_2O_4$ film was deposited on MgO and $MgAl_2O_4$ substrates by the rf-sputtering process. The films were prepared at an RF-magnetron sputtering power of 50 W and a pressure of 10 mtorr (20 sccm in Ar), and at substrate temperatures of $550^{\circ}C$. The crystal structure was determined to be a spinel (Fd-3m) structure by means of X-ray diffraction (XRD) with Cu $K{\yen}{\acute{a}}$ radiation. The thickness and morphology of the films were measured by scanning electron microscopy (SEM) and atomic force microscopy (AFM). The magnetic properties were measured using a Superconducting Quantum Interference Device (SQIUD) magnetometer. While the ferrimagnetic transitions were observed at about 93 K, which was determined as the Neel temperature, the magnetic properties all show different behaviors. The differences between the magnetic properties can be explained by the stress effects between $CoCr_2O_4$ and the substrates of MgO and $MgAl_2O_4$.

• 한국초전도ㆍ저온공학회논문지
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• 제16권4호
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• pp.36-39
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• 2014

We report on the superconducting and structural characteristics of Pb-based alloy ($Pb_{0.9}In_{0.1}$, $Pb_{0.8}In_{0.2}$ and $Pb_{0.85}Bi_{0.15}$) thin films, depending on the film deposition rate. The maximum critical magnetic field strength of $Pb_{0.85}Bi_{0.15}$ is almost six times larger than that of $Pb_{0.9}In_{0.1}$, and more rapid growth of the film enhances the critical magnetic field strength even for the same alloy material. Scanning electron microscopy inspection indicates that lower deposition rate condition is vulnerable to the formation of void structure in the film. Topographic images using atomic force microscopy are useful to optimize the deposition condition for the growth of smooth superconducting film. Our work can be utilized for future studies on hybrid superconducting devices using low-dimensional nanostructures.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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• pp.111.1-111.1
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• 2015

As an alternative way to get sophisticated nanostructures, atomic force microscopy (AFM) has been used to directly manipulate building primitives. In particular, assembly of metallic nanoparticles(NPs) can provide various structures for making various metamolecules. As far, conventionally made polygonal shaped metallic NPs showed non-uniform distribution in size and shape which limit its study of fundamental properties and practical applications. In here, we optimized conditions for deterministic manipulation of ultra-smooth and super-spherical gold nanoparticles (AuNPs) by AFM. [1] Lowered adhesion force by using platinum-iridium coated AFM tips enabled us to push super-spherical AuNPs in linear motion to pre-programmed position. As a result, uniform and reliable electric/magnetic behaviors of assembled metamolecules were achieved which showed a good agreement with simulation data. Furthermore, visualization of near field for super-spherical AuNPs was also addressed using photosensitive azo-dye polymers. Since the photosensitive azo-dye polymers can directly record the intensity of electric field, optical near field can be mapped without complicated instrumental setup. [2] By controlling embedding depth of AuNPs, we studied electric field of AuNPs in different configuration.

• 한국자기학회지
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• 제11권4호
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• pp.168-172
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• 2001

Sol-gel법을 이용하여 Co$_{0.9}$Zn$_{0.1}$Fe$_2$O$_4$ 박막을 제조하였다. 성장한 박막의 구조 및 자기적 성질에 관하여 x선 회절분석기 (XRD), atomic force microscopy(AFM) 및 Auger electron spectroscopy(AES), 진동시료자화측정기 (VSM)을 이용하였다. Co-Zn 페라이트 박막의 경우, 400 $^{\circ}C$ 이상의 열처리 온도에서 단일상의 spinel 구조만을 가지고 있으며, 아무런 방향성이 없이 성장함을 나타내고 있다. 열처리 온도가 600 $^{\circ}C$ 이하에서 성장된 박막 표면의 거칠기는 3 nm 이하였으며, 형성된 입자의 크기는 약 40nm이하임을 알 수 있었다. 또한, 40$0^{\circ}C$에서 열처리한 경우 기판에서 Si이 Co-Zn 페라이트 박막내로 확산이 거의 나타나지 않았으나, 870 $^{\circ}C$에서 열처리한 경우 계면에서 기판과 박막의 상호 확산을 확인할 수 있었다. 제작한 박막은 외부 자기장의 방향과는 무관한 등방성의 자기적 특성을 보이며, 최대 보자력은 600 $^{\circ}C$에선 열처리한 자성박막이 약 1,900 Oe을 가짐을 알 수 있었다.있었다.

• 한국자기학회지
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• 제8권6호
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• pp.350-356
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• 1998

Sol-gel법을 이용하여 합성한 자성 garnet Y3-xLaxFe5O12(x=0.0, 0.25, 0.5, 0.75, 1.0) 분말과 박막의 결정 및 자기적 성질에 관하여 X-선 회절기, atomic force microscopy(AFM), scanning electron microscopy(SEM), 진동시료자화기 (VSM)와 Mossbauer 부노강기를 이용하여 연구하엿다. X-선 회절분석 결과와 Mossbauerqnsrhkd 실험으로부터 100$0^{\circ}C$에서 열처리한 x=0.75 이하의 Y3-xLaxFe5O12 분말의 경우 모두 순수한 cubic의 garnet 구조가 형성되었음을 확인 할 수 있었으나, x=1.0인 경우는 LaFeO3상이 함께 관측되었다. Garnet 박막의 성장을 위하여 75$0^{\circ}C$에서 2시간의 열처리로 결정화를 이루었으며, 성장한 박막은 특정한 방향성 없이 성장하였음을 알 수 있었다. Mossbauer 분광기를 이용하여 측정한 결과는 산화물을 통하여 제조한 garnet 분말의 Mossbauer spectrumthk 일치함을 알 수 있었다. 전자 현미경의 측정을 통한 분말의 입자크기는 200~300nm이며, AFM의 측정으로부터 박막의 평균 표면 거칠기가 3.17nm임을 알 수 있었다. 진동시료자화기를 이용하여 측정한 garnet 분말과 박막의 자기적 특성은 전형적인 연자성의 자기적 속성을 가지며, garnet 분말의 경우 최대 포화자화 (30 emu/g)와 최소 보자력 (52 Oe)을 가짐을 알 수 있엇다. 80$0^{\circ}C$에서 열처리한 순수한 garnet 박막시료의 경우 수직 및 수평방향으로 측정한 자화곡선은 수직방향으로 측정한 자화곡선이 낮은 포화자화를 가지며 보자력은 양방향 모두 37 Oe를 나타냈다.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2007년도 The 1st International Symposium on Advanced Magnetic Materials
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• pp.196.2-196.2
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• 2007

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2007년도 The 1st International Symposium on Advanced Magnetic Materials
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• pp.171.1-171.1
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• 2007