• 응용통계연구
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• 제16권2호
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• pp.305-319
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• 2003

본 연구에서는 바이어스 필드에 의해 왜곡된 MRI 영상에 대한 분할을 위해 확장된 EM 알고리즘을 기반으로 한 통계적 접근법을 제시한다. 영상의 명암값을 자료로 하는 분할기법들은 고주파 성분의 잡음 뿐만 아니라 영상을 불균질하게 만드는 바이어스 필드라는 저주파 성분의 왜곡에 특히 취약하다. 이 문제를 해결하기 위해 본 논문에서는 잡음을 효과적으로 제어하기 위해 마코프랜덤필드가 적용된 정규혼합모형을 고려하며, 효과적인 바이어스 필드의 보정을 위해 페널티-우도를 도입하여 추정하는 방법으로 고안되었다.

• 한국초전도저온공학회지:초전도와저온공학
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• 제11권2호
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• pp.23-29
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• 2009

The unique features of HTS offer opportunities and challenges to a number of applications. In this paper we focus on NMR and MRI magnets, illustrating them with the NMR/MRI magnets that we are currently and will shortly be engaged: a 1.3 GHz NMR magnet, an "annulus" magnet, and an $MgB_2$whole-body MRI magnet. The opportunities with HTS include: 1) high fields (e.g., 1.3 GHz magnet); 2) compactness (annulus magnet); and 3) enhanced stability despite liquid-helium-free operation ($MgB_2$whole-body MRI magnet). The challenges include: 1) a large screening current field detrimental to spatial field homogeneity (e.g., 1.3 GHz magnet); 2) uniformity of critical current density (annulus magnet); and 3) superconducting joints ($MgB_2$magnet).

• Investigative Magnetic Resonance Imaging
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• 제13권1호
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• pp.1-8
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• 2009

유방 MRI는 유방 질환의 진단과 치료 분야에 최첨단 기법으로서 지난 10년 동안 유방 MRI는 연구 분야에서 임상 분야로 진화해 왔다. 따라서, 유방 MRI의 적응증과 적절한 영상을 얻는 방법, 소견을 해석하고 보고하는 법에 대한 이해가 필요하다. 유방 MRI는 양성과 악성 종괴의 감별, 유방암 환자의 수술 전 병기 결정, 수술전 항암요법에 대한 종양의 반응 평가, 유방 성형 여성의 평가 등에 사용되고 있다. 또한 유방암 고위험군 여성에서 선별 보조 검사로서 사용될 수 있다. 이러한 목적을 성공적으로 이루기 위해서는 적절한 MRI기법과 다른 유방 영상 소견과 연관 지어 해석할 수 있는 영상의학과 의사가 중요하다. 본 소고에서는 유방 MRI의 적응증, 표준화된 용어와 카테고리의 사용에 중점을 두어 기술하고자 한다.

• 한국전자파학회논문지
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• 제23권8호
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• pp.1010-1013
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• 2012

정 자장($B_0$)의 세기가 7 T(Tesla) 고자기장 MRI(Magnetic Resonance Imaging) 시스템은 정 자장의 세기가 1.5 T 또는 3 T MRI 시스템에 비하여 인가된 RF(Radio Frequency) 필드의 높은 불균질성을 보여준다. 이러한 문제점를 극복하기 위한 한 방법으로써, 관심 영역에서의 RF 자장이 균일하도록 RF 코일의 각 요소로 들어가는 최적화된 전류의 크기와 위상 값을 얻기 위해서 convex 최적화 방법이 사용된다. 이러한 방법을 7 T MRI 시스템에 다양한 RF 코일에 적용하여 각각의 $B_1^+$ 필드 값을 비교하여 그 성능을 파악하였다.

• 한국초전도ㆍ저온공학회논문지
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• 제25권4호
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• pp.75-80
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• 2023

Rare earth barium copper oxide (REBCO) materials have shown the possibility of high-temperature superconductor (HTS) magnetic resonance imaging (MRI) magnets due to their elevated transition temperature. While numerous MRI magnet designs have emerged, there is a growing emphasis on estimating the cost before manufacturing. In this paper, we propose two designs of REBCO whole-body MRI magnets: (1) 1.5 T and (2) 3.0 T, the standard center field choices for hospital use, and compare their costs based on conductor usage. The basis topology of the design method is based on discretized solenoids to enhance field homogeneity. Magnetic stress calculation is done to further prove the mechanical feasibility of their construction. Multi-width winding technique and outer notch structure are used to improve critical current characteristic. We apply consistent constraints for current margins, sizes, and field homogeneities to ensure an equal cost comparison. A graph is plotted to show the cost increase with magnetic flux growth. Additionally, we compare our designs to two additional MRI magnet designs from other publications with respect to the cost and magnetic flux, and present the linear relationship between them.

• Investigative Magnetic Resonance Imaging
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• 제23권3호
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• pp.179-201
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• 2019

Portable low-cost magnetic resonance imaging (MRI) systems have the potential to enable "point-of-care" and timely MRI diagnosis, and to make this imaging modality available to routine scans and to people in underdeveloped countries and areas. With simplicity, no maintenance, no power consumption, and low cost, permanent magnets/magnet arrays/magnet assemblies are attractive to be used as a source of static magnetic field to realize the portability and to lower the cost for an MRI scanner. However, when taking the canonical Fourier imaging approach and using linear gradient fields, homogeneous fields are required in a scanner, resulting in the facts that either a bulky magnet/magnet array is needed, or the imaging volume is too small to image an organ if the magnet/magnet array is scaled down to a portable size. Recently, with the progress on image reconstruction based on non-linear gradient field, static field patterns without spatial linearity can be used as spatial encoding magnetic fields (SEMs) to encode MRI signals for imaging. As a result, the requirements for the homogeneity of the static field can be relaxed, which allows permanent magnets/magnet arrays with reduced sizes, reduced weight to image a bigger volume covering organs such as a head. It offers opportunities of constructing a truly portable low-cost MRI scanner. For this exciting potential application, permanent magnets/magnet arrays have attracted increased attention recently. A magnet/magnet array is strongly associated with the imaging volume of an MRI scanner, image reconstruction methods, and RF excitation and RF coils, etc. through field patterns and field homogeneity. This paper offers a review of permanent magnets and magnet arrays of different kinds, especially those that can be used for spatial encoding towards the development of a portable and low-cost MRI system. It is aimed to familiarize the readers with relevant knowledge, literature, and the latest updates of the development on permanent magnets and magnet arrays for MRI. Perspectives on and challenges of using a permanent magnet/magnet array to supply a patterned static magnetic field, which does not have spatial linearity nor high field homogeneity, for image reconstruction in a portable setup are discussed.

• 대한자기공명의과학회:학술대회논문집
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• 대한자기공명의과학회 1998년도 춘계학술대회 초록집
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• pp.43-46
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• 1998

• 한국초전도ㆍ저온공학회논문지
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• 제14권1호
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• pp.44-47
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• 2012

The substantial improvement of the signal-to-noise ratio (SNR) can be achieved with small-size samples or low-field MRI system by high-temperature superconducting(HTS) RF coil. The typical HTS RF coil made of HTS thin film is expensive and is limited the coil geometry to planar surface coil. In this study, commercial Bi-2223 HTS tapes was used as RF coil for a 0.35T permanent MRI system. It has advantages of both much lower cost and easier fabrication over HTS thin film coil. SNR gain of the image obtained from the HTS RF coil over a conventional Cu RF coil at room temperature was about 2.4-fold and 1.9-fold using the spin echo pulse sequence and gradient echo pulse sequence respectively.

• 한국컴퓨터정보학회논문지
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• 제21권12호
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• pp.11-18
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• 2016

Magnetic resonance image (MRI) is widely used in brain research field and medical image. Especially, non-invasive brain activation acquired image technique, which is functional magnetic resonance image (fMRI) is used in brain study. In this study, we investigate brain activation occurred by LED light stimulation. For investigate of brain activation in experimental small animal, we used high magnetic field 9.4T MRI. Experimental small animal is Balb/c mouse, method of fMRI is using echo planar image (EPI). EPI method spend more less time than any other MRI method. For this reason, however, EPI data has low contrast. Due to the low contrast, image pre-processing is very hard and inaccuracy. In this study, we planned the study protocol, which is called block design in fMRI research field. The block designed has 8 LED light stimulation session and 8 rest session. All block is consist of 6 EPI images and acquired 1 slice of EPI image is 16 second. During the light session, we occurred LED light stimulation for 1 minutes 36 seconds. During the rest session, we do not occurred light stimulation and remain the light off state for 1 minutes 36 seconds. This session repeat the all over the EPI scan time, so the total spend time of EPI scan has almost 26 minutes. After acquired EPI data, we performed the analysis of this image data. In this study, we analysis of EPI data using statistical parametric map (SPM) software and performed image pre-processing such as realignment, co-registration, normalization, smoothing of EPI data. The pre-processing of fMRI data have to segmented using this software. However this method has 3 different method which is Gaussian nonparametric, warped modulate, and tissue probability map. In this study we performed the this 3 different method and compared how they can change the result of fMRI analysis results. The result of this study show that LED light stimulation was activate superior colliculus region in mouse brain. And the most higher activated value of segmentation method was using tissue probability map. this study may help to improve brain activation study using EPI and SPM analysis.

• 스마트미디어저널
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• 제5권1호
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• pp.44-48
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• 2016

장기추적 뇌영상 연구에서 자기공명영상장치의 노후 또는 기술 발전에 따른 업그레이드로 인해 연구기간 내 동일한 촬영 조건을 유지하기 어렵다. 특히, 자장 세기가 1.5T에서 3T로 증가한 경우가 많아, 기존 1.5T 영상을 새로운 3T 영상과 통합해서 분석에 사용하는 것이 가능한지 확인할 필요가 있다. 본 논문에서는 자장 세기와 스캔 방향이 다른 자기공명영상에서 측정한 해마 체적의 재현성을 연구 분석하였다. 실험참가자 296명의 3차원 T1 영상을 1.5와 3T 자기공명영상장치 각각에서 스캔 방향을 달리하여 획득하고 뇌영상 연구에 널리 사용되는 Freesurfer를 이용하여 실험참가자의 해마 체적을 측정하였다. 해마 체적의 영상종류 간 차이를 확인하기 위해 대응표본t-검정을 수행한 결과, 자기공명영상장치의 자장 세기와 스캔 방향에 따라 해마체적이 유의하게 차이가 있음을 확인하였다. 이런 결과는 촬영조건에 따라 측정된 해마체적이 달라질 수 있음을 의미하므로, 촬영 조건이 다른 영상을 통합 분석할 수 있는 기법의 개발이 필요하다고 판단된다.