• 제목/요약/키워드: ray number

검색결과 1,132건 처리시간 0.03초

$^{99}Mo-^{99m}TcO_4$ Generator의 감마선량 분포에 관한 연구 (A Study of Gamma-ray Distribution around the $^{99}Mo-^{99m}TcO_4$ Generator)

  • 박성옥
    • 대한방사선기술학회지:방사선기술과학
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    • 제24권1호
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    • pp.49-53
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    • 2001
  • A number of radionuclides of interest in nuclear medicine are short lived isotopes that emit only gamma ray. The most of all Dept. of Nuclear Medicine in the hospt. are using the $^{99}Mo-^{99m}Tc$ generator for elution of the short lived isotope $^{99m}TcO_4$. A $^{99}Mo-^{99m}Tc$ generator consists of an alumina column on which $^{99}Mo$ is bound. The parent isotope($^{99}Mo$ : half life 67 hr.) decays to its daughter $^{99m}TcO_4^-$ which is a different element with a shorter half-life. $^{99}Mo$ emitted 41-keV(1.3%), 141-keV(5.6%) 181-keV(6.6%) and 366-keV(1.5%) gamma rays. But $^{99m}TcO_4$ emitted only 140-keV gamma ray. We study about the gamma ray distribution around the $^{99}Mo$ generator. And obtained the result as follows ; 1. Total counted gamma ray from generator smaller in front side than back. 2. The gamma ray emitted from $^{99}Mo$ generator without $^{99m}TcO_4$ vial increased in the back side(Mo column posited side) 3. The gamma ray only from the $^{99m}TcO_4$ vial increased in the front side. 4. Apron can protect gamma ray above 60% of total radiation from the $^{99}Mo$ generator.

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차량 네트워크 시스템을 위한 노드 매핑 기반 FlexRay-CAN 게이트웨이 구현 (Implementation of Node Mapping-based FlexRay-CAN Gateway for In-vehicle Networking System)

  • 배용경;김만호;이석;이경창
    • 한국자동차공학회논문집
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    • 제19권6호
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    • pp.37-45
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    • 2011
  • As vehicles become more intelligent, in-vehicle networking (IVN) systems such as controller area network (CAN) or FlexRay are essential for convenience and safety of drivers. To expand the applicability of IVN systems, attention is currently being focused on the communication between heterogeneous networks such as body networking and chassis networking systems. A gateway based on message mapping method was developed to interconnect FlexRay and CAN networks. However, this type of gateways has the following shortcomings. First, when a message ID was changed, the gateway must be reloaded with a new mapping table reflecting the change. Second, if the number of messages to be transferred between two networks increase, software complexity of gateway increases very rapidly. In order to overcome these disadvantages, this paper presents FlexRay-CAN gateway based on node mapping method. More specifically, this paper presents a node mapping based FlexRay-CAN gateway operation algorithm along with the experimental evaluation for ID change.

X-ray Data Analysis to Search for Magnetar Candidates in the Galactic Plane

  • Park, Woochan;An, Hongjun
    • Journal of Astronomy and Space Sciences
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    • 제35권3호
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    • pp.133-141
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    • 2018
  • We report on our Galactic plane searches for magnetars in the archival Chandra X-ray Observatory (CXO) data. We summarize the properties of known magnetars and use them to establish a procedure for magnetar searches. The procedure includes four steps: source finding, spectral characterization, optical counterpart checks, and period searches. We searched 1,282 archival CXO observations, found 32,838 X-ray sources, and selected 25 intriguing candidates using the developed procedure. Although we do not firmly identify a magnetar among them, we significantly reduced the number of targets in future magnetar searches to be done with better X-ray telescopes.

매틀랩/시뮬링크 기반 플렉스레이 네트워크 시스템의 구현 및 검증 (Implementation and Verification of FlexRay Network System using Matlab/Simulink)

  • 윤승현;서석현;황성호;권기호;전재욱
    • 제어로봇시스템학회논문지
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    • 제16권7호
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    • pp.655-660
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    • 2010
  • As increasing the number of Electronic Control Units in a vehicle, the proportion for reliability and stability of the software is going increasingly. Accordingly, the traditional CAN network has occurred the situation that the requirement of developing vehicle software is not sufficient. To solve these problems, the FlexRay network which is ensured the high bandwidth and real-time is generated. However it is difficult to implement FlexRay based application software because of complex protocol than traditional CAN network. Accordingly the system for analysis and verification of network state is needed. Also vehicle vendor develops application software using Matlab/Simulink in order to increase productivity. But this development method is hard to solve the network problem of node to node. Therefore this paper implements Matlab/Simulink based FlexRay network system and verifies it through comparing with existing embedded system.

몬테 카를로 시뮬레이션을 이용한 2차원 X-선 검출기에 대한 연구 (A Study of 2-dimensional X-ray Detector using Monte Carlo Simulation)

  • 신형섭;이학재;이기성;강정원
    • 반도체디스플레이기술학회지
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    • 제9권4호
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    • pp.67-70
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    • 2010
  • X-ray absorption rate and multiplication factor of X-ray detector were calculated with Garfield code. High Z (= atomic number) was important factor to increase the absorption rate but low Z is also important to increase the multiplication. Five different gas composition were examined under the condition of 1400 V bias and 400 um gap. Xe 100% gas showed the highest absorption rate and He 96% + isobutene 4% showed the highest multiplication.

컨볼루션 뉴럴 네트워크 기반의 딥러닝을 이용한 흉부 X-ray 영상의 분류 및 정확도 평가 (Evaluation of Classification and Accuracy in Chest X-ray Images using Deep Learning with Convolution Neural Network)

  • 송호준;이은별;조흥준;박세영;김소영;김현정;홍주완
    • 한국방사선학회논문지
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    • 제14권1호
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    • pp.39-44
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    • 2020
  • 본 연구에서는 CNN과 빅데이터 기술을 이용한 Deep Learning을 통해 흉부 X-ray 영상 분류 및 정확성 연구에 대하여 알아보고자 한다. 총 5,873장의 흉부 X-ray 영상에서 Normal 1,583장, Pneumonia 4,289장을 사용하였다. 데이터 분류는 train(88.8%), validation(0.2%), test(11%)로 분류하였다. Convolution Layer, Max pooling layer pool size 2×2, Flatten layer, Image Data Generator로 구성하였다. Convolution layer가 3일 때와 4일 때 각각 filter 수, filter size, drop out, epoch, batch size, 손실함수 값을 설정하였다. test 데이터로 Convolution layer가 4일 때, filter 수 64-128-128-128, filter size 3×3, drop out 0.25, epoch 5, batch size 15, 손실함수 RMSprop으로 설정 시 정확도가 94.67%였다. 본 연구를 통해 높은 정확성으로 분류가 가능하였으며, 흉부 X-ray 영상뿐만 아니라 다른 의료영상에서도 많은 도움이 될 것으로 사료된다.

디지털유방촬영에서 Geant4-GATE를 이용한 산란선의 영향분석과 감소방안에 관한 연구 (Analysis of Scatter Ray Distribution Using GEANT4-GATE Simulation and Effectiveness of Silicone Pad in Digital Mammography)

  • 김명수;김영근;장영일
    • 대한방사선기술학회지:방사선기술과학
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    • 제42권3호
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    • pp.175-180
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    • 2019
  • In this study, we have researched the effectiveness of silicone pad. A distribution of scatter ray in mammography was evaluated using Monte-Carlo (MC) simulation technique and then a silicone pad was applied to remove the scatter ray for improving image quality. Molybdenum target and Molybdenum filter combination made a difference of 59.8% to a number of photon at 17.5 keV. On the other hand, Tungsten target and Rhodium filter showed a variation of 24.5% at 20 keV. Mean 68 of SNR was increased in Selenia and mean 1.04 of SNR was raised in Senographe. Silicone pad was significantly effective to reduce the scatter ray that was generated by primary X-ray. It can decrease an absorption rate of scatter ray to patient body and whilst it improve the image quality from increasing SNR.

잣나무와 낙엽송재 방사조직의 연륜 내 및 축방향 변이성 (Intraannual and Vertical Variations in Rays of Pinus koraiensis and Larix kaempferi Woods Grown in Korea)

  • 김남훈
    • Journal of the Korean Wood Science and Technology
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    • 제37권1호
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    • pp.65-72
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    • 2009
  • 잣나무와 낙엽송 조림목 수간 내에서 단열방사조직과 방추형방사조직의 연륜 내 및 축방향의 변이성을 조사하였다. 잣나무와 낙엽송의 단열방사조직의 높이는 각기 평균 6.3 및 9.1 세포고로서 낙엽송이 더 높았다. $0.25mm^2$ 면적당 단열방사조직의 개수는 각각 평균 6.5개 및 7.5개로써 낙엽송이 더 많았으며 방추형방사조직의 높이는 양 수종 모두 평균 20세포고 정도로서 거의 차이가 없었다. 연륜 내에서 조재부에서 만재부로 이행해 감에 따라 단열방사조직과 방추형방사조직의 높이는 감소하였으나 개수에는 거의 변화가 없었다. 축방향으로 단열방사조직의 세포고는 지상고가 증가함에 따라 점차 증가하였다. 단열방사조직의 개수는 잣나무에서 지상고 5.2m까지 거의 일정하였고 그 이상의 지상고부터 증가하였으나 낙엽송에서는 일관된 경향을 찾아보기 어려웠다. 방추형방사조직의 높이는 지상고가 낮은 수간의 기부에서 가장 낮았으며 수간의 중앙부로 올라감에 따라 높아 지다가 수관부에서 다시 낮아지는 경향이 있었다. 본 연구 결과, 연륜 내에서의 방사조직의 변이성은 비교적 뚜렷하였으나 축방향에서의 변이성은 일관된 경향이 없어 그 경향을 명확히 밝히는 것은 어려울 것으로 생각되었다.

In Situ X-ray Photoemission Spectroscopy Study of Atomic Layer Deposition of $TiO_2$ on Silicon Substrate

  • Lee, Seung-Youb;Jeon, Cheol-ho;Kim, Yoo-Seok;Kim, Seok-Hwan;An, Ki-Seok;Park, Chong-Yun
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
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    • pp.222-222
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    • 2011
  • Titanium dioxide (TiO2) has a number of applications in optics and electronics due to its superior properties, such as physical and chemical stability, high refractive index, good transmission in vis and NIR regions, and high dielectric constant. Atomic layer deposition (ALD), also called atomic layer epitaxy, can be regarded as a special modification of the chemical vapor deposition method. ALD is a pulsed method in which the reactant vapors are alternately supplied onto the substrate. During each pulse, the precursors chemisorb or react with the surface groups. When the process conditions are suitably chosen, the film growth proceeds by alternate saturative surface reactions and is thus self-limiting. This makes it possible to cover even complex shaped objects with a uniform film. It is also possible to control the film thickness accurately simply by controlling the number of pulsing cycles repeated. We have investigated the ALD of TiO2 at 100$^{\circ}C$ using precursors titanium tetra-isopropoxide (TTIP) and H2O on -O, -OH terminated Si surface by in situ X-ray photoemission spectroscopy. ALD reactions with TTIP were performed on the H2O-dosed Si substrate at 100$^{\circ}C$, where one cycle was completed. The number of ALD cycles was increased by repeated deposition of H2O and TTIP at 100$^{\circ}C$. After precursor exposure, the samples were transferred under vacuum from the reaction chamber to the UHV chamber at room temperature for in situ XPS analysis. The XPS instrument included a hemispherical analyzer (ALPHA 110) and a monochromatic X-ray source generated by exciting Al K${\alpha}$ radiation (h${\nu}$=1486.6 eV).

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CT 모의치료장치에서 발생된 X-선 빔의 유효에너지 계산식 유도 (Derivation of the Effective Energy Calculation Formula of the X-ray Beam Generated by the CT Simulator)

  • 김종언;이상훈
    • 한국방사선학회논문지
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    • 제15권6호
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    • pp.869-875
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    • 2021
  • 이 연구의 목적은 CT 모의치료장치에서 발생된 X-선 빔의 유효에너지 계산식을 유도하는데 있다. 90, 120, 140 kVp X-선 빔 하에서, AAPM CT 성능 팬텀의 CT수 교정 삽입부는 CT 모의치료장치로 5번 스캔하였다. 폴리에틸렌, 폴리스틸렌, 물, 나일론, 폴리카보네이트, 그리고 아크릴의 CT수는 각각의 CT 슬라이스 영상에 대하여 측정하였다. 단일 관전압 하에서 측정된 CT수 평균값과 미국표준기술연구소의 자료로부터 계산된 각각의 광자에너지에 대응하는 선감쇠계수들을 선형정합하였다. 얻어진 상관계수들 중 최대값을 갖는 광자에너지를 유효에너지를 결정하였다. 이와 같은 방법으로, 각각의 관전압에서 생성된 X-선 빔의 유효에너지를 결정하였다. 결정된 유효에너지(y)들와 관전압(x)들을 선형정합하여 유효에너지 계산식으로서 y=0.33026x+30.80263을 유도하였다.