• 제목/요약/키워드: neutron tomography

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중성자 토모그래피를 위한 영상처리 자체코드 개발 연구 (Research for development of our own image processing code for neutron tomography)

  • 김진만;김태주;유동인
    • 한국가시화정보학회지
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    • 제18권1호
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    • pp.44-49
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    • 2020
  • Neutron radiography has been widely used in many research areas due to its different characteristics from X-rays. Neutron tomography is a powerful tool because it can clearly show the inside of an object that the eye cannot see. However, generally, commercial software is used for the reconstruction of neutron tomography. It means that maintenance costs are incurred and analysis is inefficient in some cases. In this respect, our own image processing code is required to reconstruct neutron images efficiently. In this study, an image processing code is developed for reconstruction of cross-sectional images from neutron radiography taken from the side of the object. Using the developed code, cross-sectional images of the sample are successfully reconstructed.

Update of Neutron Science at KAERI

  • Lee, K.H.;Kim, C.J.
    • 한국초전도학회:학술대회논문집
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    • 한국초전도학회 2008년도 High Temperature Superconductivity Vol.XVIII
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    • pp.20-20
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    • 2008
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Sensing changes in tumor during boron neutron capture therapy using PET with a collimator: Simulation study

  • Yang, Hye Jeong;Yoon, Do-Kun;Suh, Tae Suk
    • Nuclear Engineering and Technology
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    • 제52권9호
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    • pp.2072-2077
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    • 2020
  • The purpose of this study was to demonstrate the feasibility of sensing changes in a tumor during boron neutron capture therapy (BNCT) using a Monte Carlo simulation tool. In the simulation, an epi-thermal neutron source and a water phantom including boron uptake regions (BURs) were simulated. Moreover, this simulation also included a detector for positron emission tomography (PET) scanning and an adaptively-designed collimator (ADC) for PET. After the PET scanning of the water phantom, including the 511 keV source in the BUR, the ADC was positioned in the PET's gantry. Single prompt gamma rays were collected through the ADC during neutron irradiation. Then, single prompt gamma ray-based tomography images of different sized tumors were acquired by a four-step process. Both the signal-to-noise ratio (SNR) and tumor size were analyzed from each step image. From this analysis, we identified a decreasing trend of both the SNR and signal intensity as the tumor size decreased, which was confirmed in all images. In conclusion, we confirmed the feasibility of sensing changes in a tumor during BNCT using PET and an ADC through Monte Carlo simulation.

Bubbly, Slug, and Annular Two-Phase Flow in Tight-Lattice Subchannels

  • Prasser, Horst-Michael;Bolesch, Christian;Cramer, Kerstin;Ito, Daisuke;Papadopoulos, Petros;Saxena, Abhishek;Zboray, Robert
    • Nuclear Engineering and Technology
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    • 제48권4호
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    • pp.847-858
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    • 2016
  • An overview is given on the work of the Laboratory of Nuclear Energy Systems at ETH, Zurich (ETHZ) and of the Laboratory of Thermal Hydraulics at Paul Scherrer Institute (PSI), Switzerland on tight-lattice bundles. Two-phase flow in subchannels of a tight triangular lattice was studied experimentally and by computational fluid dynamics simulations. Two adiabatic facilities were used: (1) a vertical channel modeling a pair of neighboring sub-channels; and (2) an arrangement of four subchannels with one subchannel in the center. The first geometry was equipped with two electrical film sensors placed on opposing rod surfaces forming the subchannel gap. They recorded 2D liquid film thickness distributions on a domain of $16{\times}64$ measuring points each, with a time resolution of 10 kHz. In the bubbly and slug flow regime, information on the bubble size, shape, and velocity and the residual liquid film thickness underneath the bubbles were obtained. The second channel was investigated using cold neutron tomography, which allowed the measurement of average liquid film profiles showing the effect of spacer grids with vanes. The results were reproduced by large eddy simulation + volume of fluid. In the outlook, a novel nonadiabatic subchannel experiment is introduced that can be driven to steady-state dryout. A refrigerant is heated by a heavy water circuit, which allows the application of cold neutron tomography.

Development of a novel reconstruction method for two-phase flow CT with improved simulated annealing algorithm

  • Yan, Mingfei;Hu, Huasi;Hu, Guang;Liu, Bin;He, Chao;Yi, Qiang
    • Nuclear Engineering and Technology
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    • 제53권4호
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    • pp.1304-1310
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    • 2021
  • Two-phase flow, especially gas-liquid two-phase flow, has a wide application in industrial field. The diagnosis of two-phase flow parameters, which directly determine the flow and heat transfer characteristics, plays an important role in providing the design reference and ensuring the security of online operation of two-phase flow system. Computer tomography (CT) is a good way to diagnose such parameters with imaging method. This paper has proposed a novel image reconstruction method for thermal neutron CT of two-phase flow with improved simulated annealing (ISA) algorithm, which makes full use of the prior information of two-phase flow and the advantage of stochastic searching algorithm. The reconstruction results demonstrate that its reconstruction accuracy is much higher than that of the reconstruction algorithm based on weighted total difference minimization with soft-threshold filtering (WTDM-STF). The proposed method can also be applied to other types of two-phase flow CT modalities (such as X(𝛄)-ray, capacitance, resistance and ultrasound).

붕소 중성자 포획 치료에서 치료 영역 영상화를 위한 예비 연구 (Preliminary Study for Imaging of Therapy Region from Boron Neutron Capture Therapy)

  • 정주영;윤도군;한성민;장홍석;서태석
    • 한국의학물리학회지:의학물리
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    • 제25권3호
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    • pp.151-156
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    • 2014
  • 본 연구의 목적은 붕소 중성자 포획 치료 시 집적된 붕소 영역에서 중성자 선속의 변화와 그에 따른 방출된 즉발 감마선의 검출 시뮬레이션을 통하여 치료 영역에 대한 영상화의 가능성을 확인하고자 함이다. 전산 모사를 통하여 (1) 붕소 유무에 따른 중성자의 영향, (2) 내부와 외부에서의 즉발 감마선량 검출, (3) 즉발 감마선에 대한 에너지 스펙트럼 검출을 수행하였다. 모든 전산 모사는 Monte Carlo n-particle extended (MCNPX, Ver.2.6.0, Los Alamos National Laboratory, Los Alamos, NM, USA)를 이용하여 가상의 물 팬텀과 열중성자(thermal neutron) 소스, 붕소 영역을 지정하였다. 열중성자의 에너지는 1 eV 이하의 에너지였으며 선속은 2,000,000 n/sec.로 설정하였다. 이 때, 발생된 즉발 감마선의 검출은 물 팬텀과 수직 방향으로 위치시키고 납으로 둘러싸인 lutetium-yttrium oxyorthosilicate (Lu0,6Y1,4Si0,5:Ce; LYSO) 섬광체 검출기를 이용하였다. 붕소가 존재하는 영역인 5 cm 깊이에서의 28 분할로서 대략 0.18 cm의 bin을 도출하여 붕소 영역의 얕은 깊이에서부터 급격하게 저하되는 것을 확인하였다. 또한 붕소 영역이 시작되는 지점인 9 cm 깊이에서 감마선의 피크 레벨을 확인하였다. 그리고 478 keV 지점에서 정확한 즉발 감마선 피크가 관찰되는 것을 확인하였다. 478 keV의 즉발 감마선 피크는 41 keV의 반치폭으로 에너지 분해능 값은 8.5%로 측정되었다. 결론적으로 붕소 중성자 포획 치료 시 발생되는 즉발 감마선의 계측으로 치료가 행해지는 부위를 감마 카메라 또는 단일 광자 방출 단층 촬영 기기에서 영상화할 수 있는 가능성을 확인하였다.

물리탐사 기법들의 화학공법 모니터링 적용성 분석 (An Analysis on Applicability of Geophysical Exploration Methods to Monitoring Polymer-flooding)

  • 천세욱;박찬호;구본진;남명진;손정술
    • 지구물리와물리탐사
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    • 제18권3호
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    • pp.143-153
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    • 2015
  • 탄화수소 생산에서 화학공법은 폴리머 용액을 저류층에 주입함으로써 탄화수소의 생산량을 증대시키는 방법이다. 화학공법의 유용성을 파악하기 위해서는 저류층 내 폴리머 용액의 거동 양상을 모니터링하는 것이 매우 중요하다. 저류층 내 폴리머 용액과 유체 변화에 대한 모니터링의 가능성을 확인하기 위해, 저류층을 구성하고 있는 암석 및 유체의 종류, 포화도 등의 매개변수에 따른 탄성파 및 전기비저항 암석물리모델을 구성하고, 폴리머 주입에 따른 탄성파 및 EM 토모그래피의 반응을 계산하였다. 특히 전기비저항 암석물리모델 구성에서는 순수사암, 셰일질 사암, 사암셰일박리층 3가지의 서로 다른 저류층 암석을 고려하였다. 폴리머 용액의 농도는 가장 일반적으로 이용되는 2 wt%로 하고 담수를 이용한 경우와 염수를 이용한 경우로 나누어 분석하였다. 더 나아가, 화학공법에 대한 중성자검층 민감도 분석을 수행하였다. 이 논문에서 다루는 기법들은 탄화수소 저류층뿐만 아니라 지열 저류층 등의 모니터링에 있어서도 중요하게 적용될 것이다.

Cross Talk Experiment with Two-element CdTe Detector and Collimator for BNCT-SPECT

  • Manabe, Masanobu;Ohya, Ryosuke;Saraue, Nobuhide;Sato, Fuminobu;Murata, Isao
    • Journal of Radiation Protection and Research
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    • 제41권4호
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    • pp.328-332
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    • 2016
  • Background: Boron Neutron Capture Therapy (BNCT) is a new radiation therapy. In BNCT, there exists some very critical problems that should be solved. One of the severest problems is that the treatment effect cannot be known during BNCT in real time. We are now developing a SPECT (single photon emission computed tomography) system (BNCT-SPECT), with a cadmium telluride (CdTe) semiconductor detector. BNCT-SPECT can obtain the BNCT treatment effect by measuring 478 keV gamma-rays emitted from the excited state of $^7Li$ nucleus created by $^{10}B(n,{\alpha})$ $^7Li$ reaction. In the previous studies, we investigated the feasibility of the BNCT-SPECT system. As a result, the S/N ratio did not meet the criterion of S/N > 1 because deterioration of the S/N ratio occurred caused by the influence of Compton scattering especially due to capture gamma-rays of hydrogen. Materials and Methods: We thus produced an arrayed detector with two CdTe crystals to test cross talk phenomenon and to examine an anti-coincidence detection possibility. For more precise analysis for the anti-coincidence detection, we designed and made a collimator having a similar performance to the real BNCT-SPECT. Results and Discussion: We carried out experiments with the collimator to examine the effect of cross talk of scattering gamma-rays between CdTe elements more practically. As a result of measurement the coincidence events were successfully extracted. Conclusion: We are now planning to carry out evaluation of coincidence rate from the measurement and comparison of it with the numerical calculations.