• 대한기계학회논문집A
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• 제37권4호
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• pp.511-519
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• 2013

능동 자기베어링의 바이어스 선형화 방법은 자기베어링의 동역학적 성능과 선형성을 확보하지만, 바이어스 전류에 의한 상시 소모전력이 발생하여 시스템의 효율이 저하된다. 반면, 스위칭 제어기는 바이어스 전류를 사용하지 않아 베어링의 소비 전력을 최소화할 수 있다. 본 논문에서는 능동 자기베어링 시스템에 적용되는 스위칭 제어기와 동기 노치필터를 포함하는 비례-미분 제어기의 성능을 비교하였다. 공정하고 객관적인 비교를 위해 기준제어기인 동기 노치필터 제어기를 합리적으로 설계하고, 스위칭 제어기가 기준제어기와 동일한 동역학 특성을 갖도록 하였다. 회전축의 굽힘 유연모드 및 센서와 증폭기의 특성을 포함하는 시스템의 동역학 모델을 수립하고 성능 비교 지표를 수립하였다. 불평형 질량에 응답 측면에서 제어기를 비교하여, 저속 영역에서 스위칭 제어기가 기준제어기 대비 10 배 이상 동손을 저감할 수 있으나, 회전축의 굽힘 유연모드와 일치하는 회전 속도 근방에서는 스위칭 제어기가 유효하지 않음을 확인하였다.

• 전기학회논문지
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• 제62권9호
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• pp.1324-1328
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• 2013

The reason of train location detection is generally the train interval control between the railway stations and the train path control in the railway station yard in order to avoid train collision. It is very important to know the train location for shortening the train headway, and improving the efficiency of railway maintenance as well as the safe operation of trains. Therefore, the accurate detection of train location is the prerequisite technology in railway signalling system. The track circuit and the wheel sensor of rolling stock have been used to detect the train location widely in urban railway as well as high speed train. The track circuit is continuously monitored by electrical equipment to detect the absence of the train and the tachometer and encoder is used for the wheel sensor to measure the train speed. But speed sensor failures are frequent due to the extremely harsh operating conditions encountered in rail vehicle. The CBTC(Communication based Train Control) system has been used in urban railway system recently. But the installation of CBTC system is very high and the modification of design is difficult. This paper deals with the feasibility of new train location detection method using magnetic sensors.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.370.1-370.1
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• 2014

Giant magnetoresistance (GMR), tunneling magnetoresistance (TMR), and magnetic random-access memory (MRAM) are currently active areas of research. Magnetite, Fe3O4, is predicted to possess as half-metallic nature, ~100% spin polarization (P), and has a high Curie temperature (TC~850 K). On the other hand, Spinel ferrite CoFe2O4 has been widely studies for various applications such as magnetorestrictive sensors, microwave devices, biomolecular drug delivery, and electronic devices, due to its large magnetocrystalline anisotropy, chemical stability, and unique nonlinear spin-wave properties. Here we have investigated the magneto-transport properties of epitaxial CoxFe3-xO4 thin films. The epitaxial CoxFe3-xO4 (x=0; 0.4; 0.6; 1) thin films were successfully grown on MgO (100) substrate by molecular beam epitaxy (MBE). The quality of the films during growth was monitored by reflection high electron energy diffraction (RHEED). From temperature dependent resistivity measurement, we observed that the Werwey transition (1st order metal-insulator transition) temperature increased with increasing x and the resistivity of film also increased with the increasing x up to $1.6{\Omega}-cm$ for x=1. The magnetoresistance (MR) was measured with magnetic field applied perpendicular to film. A negative transverse MR was disappeared with x=0.6 and 1. Anomalous Hall data will be discussed.

• 센서학회지
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• 제8권6호
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• pp.427-433
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• 1999

본 논문은 페라이트 코어, 여자코일과 픽업코일로 구성된 1축 fluxgate 마그네틱 센서를 제안하였다. 본 마그네토미터는 검출소자, 여자코일을 위한 드라이브 회로, 픽업코일 출력으로부터 DC 자장에 비례한 제 2고조파 성분검출을 위한 신호처리 회로로 구성하여 회로를 설계하고 제작하였다. 코어는 82회의 여자코일을 통해 구형파전압으로 여자하였다. 픽업 코일(150 회)의 제 2고조파 출력은 FFT 스펙트럼 분석기로 측정하였으며, 그 결과를 제 2 고조파 성분 검출을 위한 PSD(phase sensitive detector)단의 출력과 비교하였다. 감도는 구동주파수 2 (kHz)에서 약 50 [V/T]의 결과를 얻었으며, fluxgate 마그네틱 센서의 비선형계수는 약 2.0% 정도였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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• pp.331-332
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• 2008

Couplings between electric, magnetic, and structural order parameters result in the so-called multiferroic phenomena with two or more ferroic phenomena such as ferroelectricity, ferromagnetism, or ferroelasticity. The simultaneous ferroelectricity and ferromagnetism (magnetoelectricity) permits potential applications in information storage, spintronics, and magnetic or electric field sensors. The perovskite BiFeO3(BFO) is known to be antiferromagnetic below the Neel temperature of 647K and ferroelectric with a high Curie temperature of 1043K. It exhibits weak magnetism at room temperature due to the residual moment from a canted spin structure. It is likely that non-stoichiometry and second-phase formation are the factors responsible for leakage current in BFO. It has been suggested that oxygen non-stoichiometry leads to valence fluctuations of Fe ions in BFO, resulting in high conductivity. To reduce the large leakage current of BFO, one attempt is to make donor-doped BFO compounds and thin films. In this study, (Bi1-x,Ndx)(Fe1-y,Tiy)O3 thin films have been deposited on Pt(111)/TiO2/SiO2/Si substrates by pulsed laser deposition. The effect of dopants on the phase evolution and surface morphology are analyzed. Furthermore, electrical and magnetic properties are measured and their coupling characteristics are discussed.

• 한국자기학회지
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• 제8권4호
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• pp.231-240
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• 1998

고밀도 자성박막헤드 및 센서용 3층 자기저항소자의 제작 및 재생신호특성에 대해 연구하였다. 컴퓨터계산모형에 의해 설계된 3층 자기저항소자의 자기저항곡선은 외부자장 -15~+22 Oe 이상에서 포화되었으며, 이 곡선은 약 4 Oe 정도 선형화영역으로 이동되었다. 실제 제작된 소자에서 자기저항곡선은 외부자장 $\pm$15 Oe 이상에서 포화되었으며, tyjs형화 영역으로 4 Oe 만큼 이동되었다. 실제소자와 계산모형에서의 MR 반응곡선은 서로 잘 일치함을 보였다. 또한 실제소자에서 재생출력신호의 실험결과는 외부자장 $\pm$4 Oe 범위 내에서 정현파를 유지하였다. 이 자장 범위 내에서 3층 자기저항소자로 제작된 헤드는 양호한 재생출력특성을 나타낼 것으로 판단된다. 이는 박막물성을 제어하는 진공증착기술과 소자제작의 효율적인 제조공정으로 사용하는데 유익할 것이다.

• 대한의용생체공학회:의공학회지
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• 제27권4호
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• pp.154-163
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• 2006

A 64-channel magnetocardiogram (MCG) system using low-noise superconducting quantum interference device (SQUID) planar gradiometers was developed for the measurements of cardiac magnetic fields generated by the heart electric activity. Owing to high flux-to-voltage transfers of double relaxation oscillation SQUID (DROS) sensors, the flux-locked loop electronics for SQUID operation could be made simpler than that of conventional DC SQUIDs, and the SQUID control was done automatically through a fiber-optic cable. The pickup coils are first-order planar gradiometers with a baseline of 4 em. The insert has 64 planar gradiometers as the sensing channels and were arranged to measure MCG field components tangential to the chest surface. When the 64-channel insert was in operation everyday, the average boil-off rate of the dewar was 3.6 Lid. The noise spectrum of the SQUID planar gradiometer system was about 5 fT$_{rms}$/$\checkmark$Hz at 100 Hz, operated inside a moderately shielded room. The MCG measurements were done at a sampling rate of 500 Hz or 1 kHz, and realtime display of MCG traces and heart rate were displayed. After the acquisition, magnetic field mapping and current mapping could be done. From the magnetic and current information, parameters for the diagnosis of myocardial ischemia were evaluated to be compared with other diagnostic methods.

• 방사선산업학회지
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• 제9권3호
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• pp.143-151
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• 2015

A PET-MR system is particularly useful in diagnosing brain diseases. We have developed a prototype positron emission tomography (PET) system which can be inserted into the bore of a whole-body magnetic resonance imaging (MRI) system that enables us to obtain PET and MRI images simultaneously with a reduced cost. Silicon photomultipliers (SiPM) are appropriated as a PET detector at PET/MR system because detectors have a high gain and are insensitive to magnetic fields. Despite of its improved performance compared to that of PMT-based detectors, there is a problem of the photo-peak channel shift which is due to the increase of the temperature inside the ring detector. This problem will occur decreasing sensitivity of the PET and image distortion. In this paper, I quantitative analyze parameters of the KAIST SiPM depending on temperature by experiments. And I designed cooling methods in consideration of the degradation of sensors for correction of the temperature in the PET gantry. According to this research, we expect that distortive images and degradation of the sensitivity will not be occurred with using the above idea to reduce heat even if the PET system operates for a long time.

• Journal of Magnetics
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• 제21권4호
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• pp.509-515
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• 2016

We report on development of a ground-based bi-axial Search-Coil Magnetometer (SCM) designed to measure time-varying magnetic fields associated with magnetosphere-ionosphere coupling processes. The instrument provides two-axis magnetic field wave vector data in the Ultra Low Frequency or ULF (1 mHz to 5 Hz) range. ULF waves are well known to play an important role in energy transport and loss in geospace. The SCM will primarily be used to observe generation and propagation of the subclass of ULF waves. The analog signals produced by the search-coil magnetic sensors are amplified and filtered over a specified frequency range via electronics. Data acquisition system digitizes data at 10 samples/s rate with 16-bit resolution. Test results show that the resolution of the magnetometer reaches $0.1pT/{\sqrt{Hz}}$ at 1 Hz, and demonstrate its satisfactory performance, detecting geomagnetic pulsations. This instrument is scheduled to be installed at the Korean Antarctic station, Jang Bogo, in the austral summer 2016-2017.

• 센서학회지
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• 제1권1호
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• pp.23-34
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• 1992

자기-저항 센서를 제작하기 위하여 Fe-Ni 합금과 Co-Ni 합금을 슬라이드 그라스와 Si wafer에 진공 증착하여 sensor element를 제작한 후 포화자속밀도($B_{s}$), 보자력($H_{c}$), 자기-저항 변화율 등을 조사하였다. 진공 증착된 Fe-Ni 합금 박막의 포화자속밀도는 0.65T이었으며 자화주파수 1 kHz에서 보자력은 0.379A/cm이었고 자냉처리 후 종방향 보자력은 0.370Acm(//), 횡방향 보자력은 0.390Acm(${\bot}$)로 변화되었다. 자기-저항 변화율은 박막의 산화로 인하여 매우 불안정하였다. 진공 증착된 Co-Ni 박막의 포화자속밀도는 0.66T이었으며 자냉처리 후의 종방향 보자력은 5.895Acm(//)이었고 횡방향 보자력은 5.898A/cm(${\bot}$)이었다. 한편 자기-저항 변화율(${\Delta}R/R$)은 $3.6{\sim}3.7%$로써 실온에서 매우 안정하였다. Fe-Ni 박막은 화학친화력이 강하여 자기-저항 센서 제조 공정에서 많은 문제점을 야기시키고 있으나, Co-Ni 박막은 화학친화력이 작고 자기-저항 효과가 뚜렷하여 고온용 자기-저항 소자 개발용 재료로 매우 적합할 것으로 사료된다.