• 한국자기학회:학술대회 개요집
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• 한국자기학회 2000년도 International Symposium on Magnetics The 2000 Fall Conference
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• pp.200-206
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• 2000

We have investigated the activation magnetic moment, which characterizes the basis magnetic moment acting as a single magnetic particle during magnetization reversal. The activation magnetic moment was measured from each local area on continuous ferromagnetic thin films, by analyzing the magnetic field dependence of magnetization reversal of the corresponding local area based on a thermally activated relaxation process. It was found that the activation magnetic moment was nonuniform on submicrometer scale; the fluctuation increased with increasing the number of layers in Co/Pd multilayers. The distribution could be well analyzed by exp($\delta$m$\^$3/2/), where $\delta$m is the deviation of the activation magnetic moment from the mean value.

• Journal of Magnetics
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• 제6권2호
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• pp.70-72
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• 2001

We have investigated the activation magnetic moment, which characterizes the basic magnetic moment acting as a single magnetic particle during magnetization reversal. The activation magnetic moment was measured from each local area on continuous ferromagnetic thin films, by analyzing the magnetic field dependence of magnetization reversal of the corresponding local area, based on a thermally activated relaxation process. It was found that the activation magnetic moment was nonuniform on a submicrometer scale; the fluctuation increased with increasing the number of layers in Co/Pd multilayers. The distribution could be well described by exp($\delta m^{3/2}$), where $\delta$m is the deviation of the activation magnetic moment from the mean value.

• 한국의학물리학회지:의학물리
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• 제17권2호
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• pp.61-66
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• 2006

상자성 복합체의 분자량에 따른 물분자의 T1 및 T2 자기이완 특성을 조사해 보고자 하였다. DMF (15 ml)와 DTPA-bis-anhydride (0.71 g, 2 mmol) 용액에 4-aminomethylcyclohexane carboxyilc acid를 넣어 리간드를 합성한 후 $Gd_2O_3$ (0.18g, 0.5 mmol)을 넣어 최종적인 Gd 착화물을 합성하였다. 상자성 복합체의 자기이완율을 측정하기 위해 상자성 복합체를 3차 증류수를 사용하여 1 mM로 희석시켰으며 1.5T(64 MHz)에서 자기이완 시간을 측정하였다. T1 자기이완시간을 측정하기 위하여 반전 회복(Inversion-recovery) 펄스열을 사용하였다. 반전 회복 펄스열의 경우 반전시간(Inversion time, T1)은 50 msec에서부터 최대 1,750 msec까지 총 35개의 반전시간에서 영상을 획득하였다. T2 자기이완시간은 CPMG(Carr-Purcell-Meiboon-Gill) 펄스열을 사용하였다. 자기이완 시간을 구하기 위해 각각의 샘플에 관심영역(region of Interest)을 설정하여 영상의 신호강도를 측정한 후 비선형 곡선 맞춤을 실행하여 T1 및 T2값을 얻어낸 후, 이를 통해서 R1 및 R2를 계산하였다. 분자량이 587 달톤인 Omniscan의 1.5T에서의 T1, T2값이($205.1{\pm}2.57$) msec, ($209.4{\pm}4.28$) msec 임에 비해 새로이 합성된 상자성 Gd 화합물의 경우 모두 T1, T2값이 T1의 경우 분자량에 따라 $(96.35{\pm}2.04)-(79.38{\pm}1.55)$ msec, T2의 경우 $(91.02{\pm}2.08)-(76.66{\pm}1.84)$ msec로 감소한 결과를 얻었다. 새로이 합성된 Gd 화합물 간에도 분자량에 따라 R1 및 R2값이 증가하는 경향을 나타내었다. 상자성 복합체의 분자량이 증가함에 따라 T1 및 T2 자기이완 시간이 단축되고 결과적으로 자기이완율 R1, R2가 분자량에 비례하여 증가하였다.

• 한국농업기계학회:학술대회논문집
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• 한국농업기계학회 2001년도 동계 학술대회 논문집
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• pp.371-378
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• 2001

• 대한자기공명의과학회:학술대회논문집
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• 대한자기공명의과학회.한국자기공명학회 2005년도 공동학술대회
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• pp.55-55
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• 2005

• Bulletin of the Korean Chemical Society
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• 제14권3호
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• pp.392-398
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• 1993

• 한국재료학회지
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• 제26권1호
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• pp.35-41
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• 2016

The electrical transport properties of $La_{0.5}Sr_{0.5}CrO_3$ below room temperatures were investigated by dielectric, dc resistivity, magnetic properties and thermoelectric power. Below $T_c$, $La_{0.5}Sr_{0.5}CrO_3$ contains a dielectric relaxation process in the tangent loss and electric modulus. The $La_{0.5}Sr_{0.5}CrO_3$ involves the transition from high temperature thermal activated conduction process to low temperature one. The transition temperature corresponds well to the Curie point. The relaxation mechanism has been discussed in the frame of electric modulus spectra. The scaling behavior of the modulus suggests that the relaxation mechanism describes the same mechanism at various temperatures. The low temperature conduction and relaxation takes place in the ferromagnetic phase. The ferromagnetic state in $La_{0.5}Sr_{0.5}CrO_3$ indicates that the electron - magnon interaction occurs, and drives the carriers towards localization in tandem with the electron - lattice interaction even at temperature above the Curie temperature.

• Journal of Magnetics
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• 제11권4호
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• pp.189-194
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• 2006

The recent development of bio-conjugated magnetic nanoparticles offers many opportunities for applications in the field of biomedicine. In particular, the use of magnetic nanoparticles for biosensing has generated widespread research efforts following the progress of various magnetic field sensors. Here we demonstrate substrate-free biosensing approaches based on the Brownian rotation of ferromagnetic nanoparticles suspended in liquids. The signal transduction is through the measurement of the magnetic ac susceptibility as a function of frequency, whose peak position changes due to the modification of the hydrodynamic radius of bio-conjugated magnetic nanoparticles upon binding to target bio-molecules. The advantage of this approach includes its relative simplicity and integrity compared to methods that use substrate-based stray-field detectors.

• 지구물리와물리탐사
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• 제15권4호
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• pp.235-244
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• 2012

석유탐사에서 자기공명검층은 저류층 내 유체의 양과 특성을 측정 및 평가 할 수 있는 물리검층 방법 중 하나로 평가되고 있다. 자기공명검층은 수소 원자의 자기모멘트와 외부 자기장을 이용하여 이 둘의 반응 즉, 분극과 이완을 측정, 분석하는 물리검층 방법이다. 측정된 자료는 저류층 내 유체의 수소밀도에 대한 정보와 감쇠 속도에 대한 정보를 포함 하고 있으며, 이를 바탕으로 적절한 자료 처리 과정을 거치면, 유체의 특성 및 유체의 양과 같은 저류층의 생산성과 관련된 중요한 정보를 취득할 수 있다. 뿐만 아니라 자기공명검층 결과를 이용한 투수성, 습윤성와 같은 생산공학적 측면의 해석방법에 대한 연구 또한 활발하게 진행되고 있다. 이 논문에서는 자기공명반응의 기본적인 이론과 자기공명검층의 역사 그리고 자기공명검층 장비를 통한 자료의 측정 원리에 대해 순서대로 알아보도록 하겠다. 또한 랜덤워크를 이용한 자기공명반응의 시뮬레이션에 대해서도 간략하게 소개하고자 한다.

• 천문학회보
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• 제39권1호
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• pp.72.1-72.1
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• 2014

In this study, we extrapolate a nonlinear force-free field (NLFFF) from an observed photospheric magnetic field to understand the three-dimensional (3D) coronal magnetic field producing a huge solar flare. The purpose of this study is to develop a NLFFF extrapolation code based on the so-called MHD relaxation method and check how accurately our model reconstructs a coronal field. Furthermore, we apply it to the photospheric magnetic field obtained by Helioseismic and Magnetic Imager (HMI) on board Solar Dynamics Observatory (SDO) to reconstruct a 3D magnetic structure. We first investigate factors in controlling the accuracy of our NLFFF code by using a semi-analytical solution obtained by Low & Lou (1990). To extend a work done by Inoue et al. (2014), we apply various boundary conditions at the side and top boundaries in order to make our solution close to a realistic solution. As a consequence, our solution has a good accuracy when three components of a reference field are all fixed at the boundaries. Furthermore, it is also found that our solution is well matched to the Low & Lou solution in the central area of a simulation domain when the three components of a potential field are fixed at side and top boundaries (this approach is close to a realistic solution). Finally, we present the 3D coronal magnetic field producing an X 1.5-class flare in the active region 11166 through the extrapolation from SDO/HMI.