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      • KCI등재

        몬테카를로 시뮬레이션을 통한 4π 컴프턴 억제 분광기 연구

        장은성,이효영,Jang, Eun-Sung,Lee, Hyo-Yeong 한국방사선학회 2017 한국방사선학회 논문지 Vol.11 No.3

        Compton suppression system은 스펙트럼에서 Compton continuum으로 존재하는 영역을 억제하는 장치 이다. 본 연구에서는 HPGe-NaI(TI)의 기하학적인 구조 파악 및 이동에 따른 이 때 그 효과를 최적화 할 수 있는 배치구조를 찾기 위하여, Monte Carlo simulation을 통해 Compton suppression의 행태적 특성을 파악하고, 몇 가지 배치구조에 대한 비교를 해보았다. 또한 거리에 따른 효율을 이용하여 환경 측정에 사용되는 실린더 비커에 적용해 보았다. ARF 값은 81.1 keV의 경우 약 1.65, 1332.4 에너지의 경우 약 1.9 정도로 나타내는 것을 확인할 수 있다. NaI(Tl) 검출기들의 위치 이동에 따라 특정한 영역에서 suppression이 일어나는 확인할 수 있다. Compton suppression system 구성의 목적에 비추어 볼 때, 결과 에너지 스펙트럼의 Compton continuum 영역 전반에 걸쳐 suppression이 이루어지는 것이 더욱 적절한 배치구조가 됨을 알 수 있다. 따라서 최적화된 구조를 통해 다양한 환경시료 측정에 적용할 수 있음을 확인 하였다. Compton suppression apparatus using the Compton scattering response, by inhibiting part of the spectrum Compton continuum Compton continuum in the area of the peak analysis of the gamma rays that enables a clearer device. In order to find out the geometry structure of high-purity germanium detector(HPGe) -NaI(TI) and to optimize the effect of movement, Monte Carlo simulation was used to grasp the behavioral characteristics of Compton suppression and compare several layout structures. And applied to the cylinder beaker used for the environmental measurement by using the efficiency according to the distance. For the low-energy source such as 81 keV, the Compton continuum is scarcely developed and the suppression effect is also insignificant because the scattering cross-section of the Compton effect is relatively low. In the spectrum for the remaining energy, it can be seen that the Compton continuum part is suppressed in a certain energy range. Compton suppression effect was not significantly different from positional shift. average reduction factor(ARF) value was about 1.08 for 81 keV and about 1.23 for 1332.4keV energy at the highest value. It can be seen that suppression over the Compton continuum region of the energy spectrum is a more appropriate arrangement. Therefore, it can be applied to various environmental sample measurement through optimized structure.

      • 호흡동조방사선 치료 시 종양 치료의 정확도 평가

        장은성,강수만,이철수,강세식,Jang, Eun-Sung,Kang, Soo-Man,Lee, Chol-Soo,Kang, Se-Sik 대한방사선치료학회 2010 대한방사선치료학회지 Vol.22 No.2

        Purpose: To evaluate the accuracy of a target position at static and dynamic state by using Dynamic phantom for the difference between tumor's actual movement during respiratory gated radiation therapy and skin movement measured by RPM (Real-time Position Management). Materials and Methods: It self-produced Dynamic phantom that moves two-dimensionally to measure a tumor moved by breath. After putting marker block on dynamic phantom, it analyzed the amplitude and status change depending on respiratory time setup in advance by using RPM. It places marker block on dynamic phantom based on this result, inserts Gafchromic EBT film into the target, and investigates 5 Gy respectively at static and dynamic state. And it scanned investigated Gafchromic EBT film and analyzed dose distribution by using automatic calculation. Results: As a result of an analysis of Gafchromic EBT film's radiation amount at static and dynamic state, it could be known that dose distribution involving 90% is distributed within margin of error of 3 mm. Conclusion: As a result of an analysis of dose distribution's change depending on patient's respiratory cycle during respiratory gated radiation therapy, it is expected that the treatment would be possible within recommended margin of error at ICRP 60.

      • GafChromic $EBT^{(R)}$ 필름을 이용한 뇌정위방사선치료의 선량분석 가능성 평가

        장은성,이철수,Jang, Eun-Sung,Lee, Chul-Soo 대한방사선치료학회 2007 대한방사선치료학회지 Vol.19 No.1

        Purpose: We have performed SRS (stereotactic radiosurgery) for avm (arterry vein malformation) and brain cancer. In order to verify dose and localization of SRS, dose distributions from TPS ($X-Knife^{(R)}$ 3.0, Radionics, USA) and GafChromic $EBT^{(R)}$ film in a head phantom were compared. Materials and Methods: In this study, head and neck region of conventional humanoid phantom was modified by substituting one of 2.5 cm slap with five 0.5 cm acrylic plates to stack the GafChromic $EBT^{(R)}$ film slice by slice with 5 mm intervals. Four films and five acrylic plates were cut along the contour of head phantom in axial plane. The head phantom was fixed with SRS head ring and adapted SRS localizer as same as real SRS procedure. CT images of the head phantom were acquired in 5 mm slice intervals as film interval. Five arc 6 MV photon beams using the SRS cone with 2 cm diameter were delivered 300 cGy to the target in the phantom. Ten small pieces of the film were exposed to 0, 50, 100, 200, 300, 400, 500, 600, 700, 800, 900 cGy, respectively to calibrate the GafChromic $EBT^{(R)}$ film. The films in the phantom were digitized after 24 hours and its linearity was calibrated. The pixel values of the film were converted to the dose and compared with the dose distribution from the TPS calculation. Results: Calibration curve for the GafChromic $EBT^{(R)}$ film was linear up to 900 cGy. The R2 value was better than 0.992. Discrepancy between calculated from $X-Knife^{(R)}$ 3.0 and measured dose distributions with the film was less than 5% through all slices. Conclusion: It was possible to evaluate every slice of humanoid phantom by stacking the GafChromic EBT film which is suitable for 2 dimensional dosimetry, It was found that film dosimetry using the GafChromic $EBT^{(R)}$ film is feasible for routine dosimetric QA of stereotactic radiosurgery.

      • 인체팬톰을 이용한 2D-3D 정합시 타켓위치의 정확성 평가

        장은성,강수만,이철수,Jang, Eun-Sung,Kang, Soo-Man,Lee, Chul-Soo 대한방사선치료학회 2009 대한방사선치료학회지 Vol.21 No.1

        Purpose: The aim of this study is to compare patient's body posture and its position at the time of simulation with one at the treatment room using On-board Imaging (OBI) and CT (CBCT). The detected offsets are compared with position errors of Rando Phantom that are practically applied. After that, Rando Phantom's position is selected by moving couch based on detected deviations. In addition, the errors between real measured values of Rando Phantom position and theoretical ones is compared. And we will evaluate target position's accuracy of KV X-ray imaging's 2D and CBCT's 3D one. Materials and Methods: Using the Rando Phantom (Alderson Research Laboratories Inc. Stanford. CT, USA) which simulated human body's internal structure, we will set up Rando Phantom on the treatment couch after implementing simulation and RTP according to the same ways as the real radioactive treatment. We tested Rando Phantom that are assumed to have accurate position with different 3 methods. We measured setup errors on the axis of X, Y and Z, and got mean standard deviation errors by repeating tests 10 times on each tests. Results: The difference between mean detection error and standard deviation are as follows; lateral 0.4+/-0.3 mm, longitudinal 0.6+/-0.5 mm, vertical 0.4+/-0.2 mm which all within 0~10 mm. The couch shift variable after positioning that are comparable to residual errors are 0.3+/-0.1, 0.5+/-0.1, and 0.3+/-0.1 mm. The mean detection errors by longitudinal shift between 20~40 mm are 0.4+/-0.3 in lateral, 0.6+/-0.5 in longitudinal, 0.5+/-0.3 in vertical direction. The detection errors are all within range of 0.3~0.5 mm. Residual errors are within 0.2~0.5 mm. Each values are mean values based on 3 tests. Conclusion: Phantom is based on treatment couch shift and error within the average 5mm can be gained by the diminution detected by image registration based on OBI and CBCT. Therefore, the selection of target position which depends on OBI and CBCT could be considered as useful.

      • 발전된 방사선 치료에 관한 고찰

        장은성,백성민,고성진,강세식,Jang, Eun-Sung,Beak, Seong-Min,Ko, Seung-Jin,Kang, Se-Sik 대한방사선치료학회 2008 대한방사선치료학회지 Vol.20 No.2

        Purpose: The cancer treatment which uses radiation from next year when the X-ray is discovered with the fact that it is started. The radiation treatment technique for a cancer treatment is developed ceaselessly without and it is come and, with advancement of the computer and electromagnetic engineering it joins in and quickly, it was made to do a many development from radiation treatment field. Accordingly, this study is examine in the radiotherapy technique which is developed that importance to therapeutic principles and methods. Materials and Methods: We had investigated record for radiotherapy technique which is developed and we had acquired information widely at clinical experience data. Results: The cancer treatment which uses the radiation of today is repeating a dazzling development. Past the treatment which is two-dimensional it does not correspond in therapeutic objective but currently 3 dimension three-dimensional moulding treatment or centurial control radiation treatment this the fourth dimension therapeutic technique which is in parallel to be introduced the complication solution in compliance with a normal organization protection and the radiation which are a difficult problem of during that time radiation treatment possibly did. Conclusion: 3-dimensional and 4-dimensional modern radiation treatment which is developen is that corresponding in objective of radiation treatment and the evaluation that again it does thick, judges in about the cancer treatment which uses radiation with the fact that the protection of normal organization is almost become accomplished.

      • KCI등재

        효율을 적용한 마리넬리 비이커에서 HPGe 감마선 분광분석법의 동시합성보정

        장은성(Eun-Sung Jang),이효영(Hyo-Yeong Lee) 한국방사선학회 2018 한국방사선학회 논문지 Vol.12 No.5

        동시 합성 보정 효과는 검출기의 효율이 향상할 때 그리고 선원과 검출기 사이의 거리가 가까울수록 크게 나타나는 것으로 알려져 있다. 점 선원( 60 Co)을 사용하여 검출기 중심축 방향 및 방사상 방향에서 거리에 따른 변화를 주어 P/T 비를 구하여 동시합성 보정을 하였다. 따라서 본 연구에서는 중심축 및 방사상 방향에서 동시합성 보정한 값들을 혼합부피선원(450 mL CRM source)에 적용하여 P/T에 따른 전체 피크효율 변화를 Geant4과 비교하였다. 또한 검출기와 시료가 아주 밀착된 상태에서 맵핑법에서 구한 효율을 환경시료 중에서 해양 시료인 미역에 적용하여 P/T 비의 적합성을 평가하고자 한다. 500 keV 이상의 효율의 영향을 받는 에너지 영역에 1,836 keV로 보정한 효율을 적용한 결과 측정값과 보정값의 상대오차는 3.2 % peak 효율이 보정되어 잘 일치하였다. 450 mL CRM source처럼 부피가 커질수록 P/T 비는 ± 5%까지 감소하 였다. 이것은 검출기로부터 선원이 멀어짐에 따라 방출된 감마선의 산란이 많아지기 때문이며, 이처럼 P/T 변화는 동시합성 보정 피크 효율에 영향을 줌을 확인하였다. Coincidence summing correction effects are known to be greater as the efficiency of the detector increases and as the distance between the source and the detector increases. A point source( 60 Co) was used to vary the distance in the direction of the detector s center axis and in the radial direction to obtain the P/T ratio for Coincidence summing correction calibration. In this study, values for coincidence summing corrected calibration of the values in the central and radial directions were applied to the mixed volume source(450 ml CRM source) to compare the overall peak efficiency change according to P/T with Geant4. In addition, the efficiency obtained from the mapping method is applied to the seaweed, a marine sample, and the compatibility of the P/T ratio with the detector and sample very dose together. The efficiency corrected to 1,836 keV was applied to the energy zone affected by the efficiency of 500 keV and the relative error of the measured and corrected values was well matcched by the 3.2 % peak efficiency correction. As with 450 mL CRM source, the larger the volume, the lower the P/T ratio was by ±5 %. This is due to the increased scattering of gamma-rays emitted as the source becomes farther away from the detector, and this change in P/T has been confirmed to affect the Coincidence summing corrected peak efficiency.

      • KCI등재

        Evaluation of Lung Dose Using Linac Photon Beam in Geant 4 Simulation

        Eun-Sung Jang(장은성),Hyo-Yeong Lee(이효영) 한국방사선학회 2018 한국방사선학회 논문지 Vol.12 No.4

        The Geant 4 simulated the linear accelerator (VARIAN CLINAC) based on the previously implemented BEAMnrC data, using the head structure of the linear accelerator. In the 10 MV photon flux, Geant4 was compared with the measured value of the percentage of the deep dose and the lateral dose of the water phantom. In order to apply the dose calculation to the body part, the actual patient s lung area was scanned at 5 mm intervals. Geant4 dose distributions were obtained by irradiating 10 MV photons at the irradiation field (5 × 5 cm2) and SAD 100 cm of the water phantom. This result is difficult to measure the dose absorbed in the actual lung of the patient so the doses by the treatment planning system were compared. The deep dose curve measured by water phantom and the deep dose curve calculated by Geant4 were well within ± 3% of most depths except the build-up area. However, at the 5 cm and 20 cm sites, 2.95% and 2.87% were somewhat higher in the calculation of the dose using Geant4. These two points were confirmed by the geometry file of Genat4, and it was found that the dose was increased because thoracic spine and sternum were located. In cone beam CT, the dose distribution error of the lungs was similar within 3%. Therefore, if the contour map of the dose can be directly expressed in the DICOM file when calculating the dose using Geant4, the clinical application of Geant4 will be used variously Geant4 코드는 직선 가속기의 헤드 구조를 사용하여 이전에 구현된 BEAMnrC 데이터를 기반으로 선형 가속기 (VARIAN CLINAC.)를 시뮬레이션하였다, 10MV 광자 선속에서 물팬텀의 심부선량백분율과 측면 선량의 측정값과 Geant4를 비교 평가하였다. 선량 계산을 인체부위에 적용하기 위해 실제 환자의 Lung 부위를 5mm 간격으로 스캔하였다. Water phantom의 조사야(5×5cm 2 ), SAD 100cm에서 10MV 광자를 조사하여 Geant4 선량분포를 구하였다. 이 결과는 실제 환자의 폐(lung)에 흡수되는 선량을 측정하기는 어렵다 그래서 치료계획 시스템에 의한 선량을 비교하였다. 물 팬텀에서 측정된 심부선량 곡선과 Geant4에 의해 계산된 심부선량 곡선은 build-up 영역을 제외한 대부분의 깊이에서 ± 3% 이내로 잘 일치하였다. 그러나 5cm와 20 cm 지점에서 2.95%와 2.87%로 Geant4를 사용한 선량 계산에서 다소 높은 값을 보이고 있다. 이 두 지점은 Genat4의 geometry 파일을 통해 확인할 수 있었으며, 흉추와 흉골이 위치되어 선량이 증가된 것으로 알 수 있었다. 또한, cone beam CT를 적용한 결과에서 폐(lung)의 선량분포 오차는 3% 이내로 유사한 값을 얻었다. 따라서 Geant4를 이용하여 선량을 계산할 때 DICOM 파일에 직접 선량의 contour map이 표현될 수 있다면 Geant4의 임상적 적용이 다양하게 사용될 것이다.

      • KCI등재

        Geant4/Gate 코드를 사용한 인체 팬텀 연구

        장은성(Eun-Sung Jang),최지훈(Ji-Hoon Choi) 한국방사선학회 2020 한국방사선학회 논문지 Vol.14 No.5

        Geant4는 C++ 언어사용에서 windows 운영체계와 호환이 가능해져, DICOM이나 소프트웨어를 연계하는 인터페이스 기능이 가능해졌다. 기하학적 고형물에 의해 인체 장기를 나타내는 팬텀은 치료나 진단에서 선량 계획과 같은 의학 용도에 널리 사용된다 방사선 방호 목적을 위해서는 에너지가 몇 keV의 일?? 설명의 유효성을 보여주는 것일 여전히 필요하다. 본 연구에서는 Geant4 시뮬레이션을 통해 저 keV부터 고 keV까지 다양하게 에너지를 선택하여 인간 팬텀중 일부분을 선택하여 광자 병렬 평면 필드에서 조사했을 때 그 장기에 대한 방사선량을 구하고 Zankl의 승인된 방법에 의해 얻은 결과에 대해 결과를 비교 검증하고자 한다. 몬테카롤로 코드를 사용하여 장기 선량을 평가하는 것의 중요성은 시뮬레이션의 다양한 묘사 및 특성에 의해 중성자, 양성자, 파온 등과 같은 빔의 여러 가지 유형의 입자와 Gev와 같은 높은 에너지에도 적합하다는 것을 확인하였다. Geant4 is compatible with the Windows operating system in C++ language use, enabling interface functions that link DICOM or software. It was simulated to address the basic structure of the simulation using Geant4/Gate code and to specifically verify the density composition and lung cancer process in the human phantom. It was visualized using the Gate Graphic System, i.e. openGL, Ray Tracer: Ray Tracing by Geant4 Tracing, and using Geant4/Gate code, lung cancer is modeled in the human phantom area in 3D, 4D to verify the simulation progress. Therefore, as a large number of new functions are added to the Gate Code, it is easy to implement accurate human structure and moving organs.

      • KCI등재

        Linac 기반 VMAT 정위적 수술 뇌 병변 연구와 기존의 정위적 방사선 수술 비교

        장은성(Eun-Sung Jang),장보석(Bo-Seok Chang) 한국방사선학회 2021 한국방사선학회 논문지 Vol.15 No.2

        기존 연구인 선량평가의 임상 적용 및 신뢰도 확보를 위하여 EPID를 이용하여 Portal Dosimetry를 검증하였다. 뇌정위방사선수술 2.5 cm cone을 장착하여 360° 회전조사에 의한 측정치와 Geant4의 선량분포를 비교하였다. 뇌전이 환자의 선량분포를 확인하기위해 두부인체 팬톰에 Gafchromic EBT필름을 삽입하여 조사한 선량분포와 VMAT을 이용한 두부인체 팬톰에서 얻은 선량분포를 비교하여 실제 환자에 적용하고자 한다. 분석결과 beam center와 couch의 center가 정확하게 일치하는가를 pin ball을 통해 QA한 결과 1 mm 이내의 오차로 정밀함을 확인할 수 있었다. 또한 EBT3 Film에 다양한 선량조사에 따라 0 ~ 10 Gy영역까지 우수한 선형성임을 확인할 수 있었다. 두경부 팬텀과 같은 설정에서 광자 빔을 사용한 Geant4에 기반한 선량 계산 도구의 구현과 시뮬레이션 결과 계산치는 치료계획용적(PTV)내에서 실험 데이터와 일치함을 확인하였다. 따라서 체적변조 아크치료(VMAT) 360° 회전 조사를 실시하여 회전조사에 의한 등선량분포 분석결과 가상 종양 을 포함하기에 적절함을 확인하였다. Portal Dosimetry was verified using EPID to secure the clinical application and reliability of the existing research dose evaluation. The dose distribution of Geant4 was compared with the measured value by 360° rotational irradiation with a 2.5 cm cone for stereotactic brain surgery. To confirm the dose distribution of patients with brain metastasis, the dose distribution investigated by inserting a Gafchromic EBT film into the parietal phantom and the dose distribution obtained from the parietal phantom using VMAT are compared and applied to actual patients. As a result of the analysis, it was confirmed that the accuracy of the beam center and the center of the couch coincide accurately with an error within 1mm as a result of QA through a pin ball. In addition, it was confirmed that the EBT3 film has excellent linearity in the range of 0 to 10 Gy according to various dose irradiation. In the same setting as the two cervical phantoms, we confirm that the implementation and simulation results calculations of dose calculations based on Geant4 using photon beams match the experimental data within the treatment planning volume (PTV). Therefore, volume modulated arc treatment (VMAT) 360° rotational irradiation was performed, and the result of iso-dose distribution analysis by rotational irradiation confirmed that it is appropriate to include a virtual tumor.

      • KCI등재

        실린더 및 확장 소스 PENELOPE 시뮬레이션에 대한 동시합성보정 계수 유용성 평가

        장은성(Eun-Sung Jang),장보석(Bo-Seok Chang) 한국방사선학회 2021 한국방사선학회 논문지 Vol.15 No.6

        PENELOPE Code를 사용하여 에너지 및 효율 교정하기 위해 부피선원을 사용하여 PENELOPE simulation 하였다. 여기서 동시 계측 보정하여 피크 효율 및 유용성을 검증하고자 한다. 모든 부피에 대한 일치 합산 보정을 계산을 위해 먼저 실린더 및 마리넬리 비커 4개의 부피를 3개의 높이로 다시 세분화 한다. 따라서 3개의 영역에서의 동시계측보정계수와 부피선원 전체에 대한 동시계측보정계수가 출력t으로 산출하게 된다. 부피선원의 영역별 효율 정보를 포함한 검출기입력파일은 Penelope 시뮬레이션을 사용하여 획득한다. 낮은 에너지에서는 각 소스 체적(50~300 ml)에 대한 J값이 작고 높은 에너지 범위에서는 크게 증가한다. 시뮬레이션 결과 최대 4%인 50 ml 및 300 ml를 제외하고 모든 선원 부피에 대해 2.5% 이내에서 잘 일치하였다. 이는 계측 시 동시계측효과에 대한 보정이 실효성이 있음을 의미한다. 또한, 이를 기반으로 다양한 선원 및 환경시료 측정 시 검출 효율성을 개선할 수 있는 이점이 있음을 확인할 수 있다. In order to calibrate energy and efficiency using the PENELOPE Code, a PENELOPE simulation was performed using a volume source. Here, we want to verify peak efficiency and usefulness by performing simultaneous measurement and correction. calculate the coincident sum correction for all volumes, first subdivide the volumes of the cylinder and the four Marinelli beakers into three heights again. Therefore, the simultaneous measurement correction coefficient in three areas and the simultaneous measurement correction coefficient for the entire volume source are calculated as output. At low energies, the j value for each source volume (50-300 ml) is small and increases significantly in the high energy range. Simulation results showed good agreement within 2.5% for all source volumes except for 50 ml and 300 ml, which were up to 4%. This means that the correction for the simultaneous measurement effect during measurement is effective. In addition. Based on this, it can be confirmed that there is an advantage to improve the detection efficiency when measuring various sources and environmental samples.

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