• 방사선산업학회지
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• 제9권2호
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• pp.85-90
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• 2015

Purpose: Time of operation has been reduced and accuracy of operation has been improved since C-arm, which offer real-time image of patient, was introduced in operation room. However, because of the contamination of patient, C-arm could not be used more appropriately. Therefore, this study is to know factors of controlling exposure dose, image quality and the exposed dose of health professional in operation room. Materials and methods: Height of Wilson frame (bed for operation) was fixed at 130 cm. Then, Model 76-2 Phantom, which was set by assembling manual of Fluke Company, was set on the bed. Head/Spine Fluoroscopy AEC mode was set for exposure condition. According to detector size of C-arm, the absorbed dose per min was measured in the 7 steps OFD (cm) from 10 cm to 40 cm (10, 15, 20, 25, 30, 35, 40 cm). In each step of OFD, the absorbed dose per min of same diameter of collimation was measured. Moreover, using Nero MAX Model 8000, exposure dose per min was measured according to 3 step of distance from detector (20 cm, 60 cm, 100 cm). Finally, resolution was measured by CDRH Disc Phantom and magnification of each OFD was measured by aluminum stick bar. Result: According to detector size of C-arm, difference of absorbed dose shows that the dose of 20 cm OFD is 1.750 times higher than the dose of 40 cm OFD. It means that the C-arm, which has smaller size of detector, shows the bigger difference of absorbed dose per min (p<0.05). In the difference of absorbed dose in the same step of OFD (from 20 cm to 40 cm), the absorbed dose of 9 inch detect or C-arm was 1.370 times higher than 12 inch' s (p<0.05). When OFD was set to 20 cm OFD, the absorbed dose of non-collimation case was approximately 0.816 times lower than the absorbed dose of collimation cases (p<0.05). When the distance was 20 cm from detector, exposed does includes first-ray and scatter-ray. When the distance was 60 cm and 100 cm from detector, exposed does includes just scatter-ray. So, there was the 2.200 times difference of absorbed does. Finally, when OFD was increased, spatial resolution was 4 to 5 step was increased. However, low contrast resolution was not relative. Moreover, there was 1.363 times difference of magnification (p<0.05). Conclusion: When C-Arm is used, avoiding contamination of patient is more important factor than reducing exposed dose of health professional in operation room. Just controlling exposure time is just way to reduce the exposed does of workers. However, in the case, non-probability influence could be occurred. Therefore, this study proved that the exposed dose will be reduced if the factors such as using small detector size of C-arm, setting OFD from 20 cm to 25 cm and non-collimating. Moreover, dose management of C-arm in the non-interesting area will be considered additionally.

• Nuclear Engineering and Technology
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• 제54권5호
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• pp.1769-1780
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• 2022

A new method of dose calculation algorithm, called GPU-accelerated Monte Carlo and collapsed cone Convolution (GMCC) was developed to improve the calculation speed of BNCT treatment planning system. The GPU-accelerated Monte Carlo routine in GMCC is used to simulate the neutron transport over whole energy range and the Collapsed Cone Convolution method is to calculate the gamma dose. Other dose components due to alpha particles and protons, are calculated using the calculated neutron flux and reaction data. The mathematical principle and the algorithm architecture are introduced. The accuracy and performance of the GMCC were verified by comparing with the FLUKA results. A water phantom and a head CT voxel model were simulated. The neutron flux and the absorbed dose obtained by the GMCC were consistent well with the FLUKA results. In the case of head CT voxel model, the mean absolute percentage error for the neutron flux and the absorbed dose were 3.98% and 3.91%, respectively. The calculation speed of the absorbed dose by the GMCC was 56 times faster than the FLUKA code. It was verified that the GMCC could be a good candidate tool instead of the Monte Carlo method in the BNCT dose calculations.

• 대한방사선기술학회지:방사선기술과학
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• 제40권3호
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• pp.355-361
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• 2017

소아는 성인보다 장기의 방사선에 대한 감수성이 크고 성장 중이기 때문에 더 민감하다. 피폭으로 인한 부작용을 겪는 기대수명이 길기 때문에 피폭선량의 관리가 어른의 경우보다 중요하게 다뤄진다. 본 연구는 10세 팬텀을 사용하여 현재 우리나라에 권고되어 있는 5세 소아의 촬영기준과 입사표면선량의 적합성을 확인하고 추가적으로 제시된 촬영기준으로 장기흡수선량을 측정해보았다. 임상에서 사용 중인 5세와 10세의 촬영조건과 장기흡수선량, 입사표면선량을 비교하였다. 임상 5세 촬영조건이 권고촬영조건보다 약간 높으며 임상 10세 촬영조건은 많이 높게 나타났다. 또한 권고 촬영조건으로 ESD를 측정한 결과 임상 촬영조건의 ESD가 43% 높게 나타났으며 10세의 ESD는 5세의 권고 촬영조건의 ESD 보다 126% 증가를 나타냈다. 5세의 권고된 ESD와 임상 촬영조건에 의한 ESD를 비교한 결과 31.6%의 차이를 나타냈다. 5세의 권고 촬영조건과 임상 촬영조건에 의한 장기흡수선량은 큰 차이는 없으나 흉부와 골반검사에서는 차이가 컸다. 그러나 10세의 임상 촬영조건에 의한 장기흡수선량을 비교하면 월등한 차이가 있었음을 알 수 있었다. 따라서 소아의 권고 선량에 대한 더욱 세분화된 기준안이 연구되어야 할 것으로 사료된다.

• 대한핵의학회지
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• 제29권1호
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• pp.54-60
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• 1995

방사성 핵종의 체내 투여 또는 체내 오염에 의한 내부피폭 흡수선량 측정을 위하여 개발된 MIRD 씨스템을 이용하여 175mCi $^{131}I$ 치료를 받는 8명의 분화된 갑상선암의 주변림프절 전이 환자에서 전신, 위, 신장, 방광 및 골수 등의 흡수선랑을 측정하였다. 전리함 검출기와 자료저장 장치가 부착된 Eberline Smart 200 씨스템을 이용하여 전신 $^{131}I$의 시간 방사능 곡선을 얻었고, 선형 회귀분석을 하여 곡선하면적을 구한 값을 투여 방사능량(Ao)으로 나누어 체류시간($\tau$)으로 하였다. MIRDose2의 S값을 이용하여 전신흡수선량을 구하였으며 ICRP publication 53의 표준인 신장, 방광, 위의 체류시간을 이용하여, 이들 장기의 흡수선량을 구하였다. 전신 및 골수의 흡수선량은 22.4 및 25.4rad로 ICRP 최대허용선량보다 훨씬 낮았으며, 방광에 375.1, 위에 285.1rad로 심각한 증상을 초래할 정도의 선량은 아니었다. 분화된 갑상선암의 폐 및 뼈전이 환자에서 200mCi 이상 투여방사능량을 증가시킬 경우 이 방법으로 전신 및 골수 등의 흡수 선량을 평가하여 안전성을 확인할 수 있을 것으로 생각된다.

• Journal of Radiation Protection and Research
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• 제11권1호
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• pp.77-82
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• 1986

Kerma와 흡수선량 사이의 관계를 결정하는 것은 선량측정의 기본적인 문제이다. 본 연구에서는 고에너지 치료용 선형가속기의 6MV X-선과 감마치료기의 $^{60}Co$에 대한 kerma와 흡수선량을 측정하였다. 본 실험결과는 $^{60}Co$감마선에 의한 물과 알루미늄의 과도 평형 영역에서의 흡수선량이 실제적으로 kerma와 일치하였으며, 최대선량 깊이는 6MV와 $^{60}Co$에서 각각 $1.45g/cm^2$과 $0.48g/cm^2$이었다. 최대 build-up에서의 흡수선량과 표면에서의 충돌 kerma의 비($K^{att}$)는 표준 조사면에서 물과 알루미늄에 대해, 6MV인 경우는 0.949, $^{60}Co$인 경우는 0.992이었다. 이 결과는 $K^{att}$의 물질에 대한 의존성이 매우 작음을 보여준다.

• 대한치과의사협회지
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• 제58권7호
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• pp.388-397
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• 2020

Objective: The purpose of the study was to calculate the effective and absorbed organ doses of cone-beam computed tomography (CBCT) in pediatric patient using personal computer-based Monte Carlo (PCXMC) software and to compare them with those measured using thermoluminescent dosimeters (TLDs) and anthropomorphic phantom. Materials and Methods: Alphard VEGA CBCT scanner was used for this study. A large field of view (FOV) (20.0 cm × 17.9 cm) was selected because it is a commonly used FOV for orthodontic analyses in pediatric patients. Ionization chamber of dose-area product (DAP) meter was located at the tube side of CBCT scanner. With the clinical exposure settings for a 10-year-old patient, DAP value was measured at the scout and main projection of CBCT. Effective and absorbed organ doses of CBCT at scout and main projection were calculated using PCXMC and PCXMCRotation software respectively. Effective dose and absorbed organ doses were compared with those obtained by TLDs and a 10-year-old child anthropomorphic phantom at the same exposure settings. Results: The effective dose of CBCT calculated by PCXMC software was 292.6 μSv, and that measured using TLD and anthropomorphic phantom was 292.5 μSv. The absorbed doses at the organs largely contributing to effective dose showed the small differences between two methods within the range from -18% to 20%. Conclusion: PCXMC software might be used as an alternative to the TLD measurement method for the effective and absorbed organ dose estimation in CBCT of large FOV in pediatric patients.

• Nuclear Engineering and Technology
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• 제52권10호
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• pp.2334-2338
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• 2020

In recent years, 3D printing technology has received significant research attention. Additionally, 3D printing technology is being applied to study radiation dosimeters of various materials. In this study, a plastic scintillator for 3D printing was developed in a laboratory and used to manufacture a plastic scintillation dosimeter (PSD) with a shape identical to that of the ionization chamber PTW31010. The 16-mm beam of Gamma Knife® Perfexion™ was irradiated to derive the absorbed dose rates of the PSD and PTW31010; they were subsequently compared with the dose rates of the treatment plan. The differences in the dose rates of the Gamma Knife treatment plan and the absorbed dose rates of PTW31010 were within 0.87%. The difference between the dose rates of the Gamma Knife treatment plan and the absorbed dose rates of the PSD were within 4.1%. A linear fit of the absorbed dose rates of four shots involving different dose rates and irradiation angles yielded an adjusted R-square value exceeding 0.9999. A total of 10 repeated measurements were conducted for the same shot to confirm its reproducibility, with a relative error of 0.56%.

• 대한방사선기술학회지:방사선기술과학
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• 제23권1호
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• pp.97-101
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• 2000

In this study, the highly sensitive $CaSO_4:Tm$-PTFE TLDs has been fabricated for the purpose of measurement of high energy electron. $CaSO_4:Tm$ phosphor powder was mixed with polytetrafluoroethylene(PTFE) powder and moulded in a disk type(diameter 8.5 mm. thickness $90\;mg/cm^2$) by cold pressing. The absorbed dose distribution and ranges for high energy electron were measured by using the $CaSO_4:Tm$-PTFE TLDs. The ranges determined were $R_{100}=14.5mm$, $R_{50}=24.1mm$ and $R_P=31.8mm$, respectively and the beam flatness, the variation of relative dose in 80% of the field size, was 4.5%. The fabricated $CaSO_4:Tm$-PTFE TLDs nay be utilized in radiation dosimetry for personal, absorbed dose and environmental monitoring.

• Journal of Radiation Protection and Research
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• 제31권1호
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• pp.1-7
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• 2006

The measured mean activities of $^{226}Ra,\;^{232}Th,\;^{40}K\;and\;^{137}Cs$ in the soil of Bahawalpur, Bahawalnagar and Rahimyar Khan Bistricts were 32.9, 53.6, 647.4 and 1.8 Bq $kg^{-1}$. The average absorbed dose rate calculated from these activities was 74.3 nGy $h^{-1}$ and the mean annual effective dose rate was found to be 0.46 mSv $y^{-1}$. Absorbed doses to different body organs were derived from annual effective doses using tissue weighting factors. Radiation induced fatal cancer risks were assessed by using ICRP 60 Model. Estimations incurred 184deaths per year due to cancer.

• 대한방사선치료학회지
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• 제27권1호
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• pp.1-11
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• 2015

목 적 : 방사선 치료 전 종양의 정확한 위치확인을 위한 치료 전 확인영상인 2D(AP,LAT), 3D(CBCT)의 흡수선량을 평가해보았다. 대상 및 방법 : Varian 사에서 제작한 OBI(Version1.5) System, CTDI 측정 phantom및 이온chamber, 교정된 유리선량계(GD-352M)를 이용하여 두부, 흉부, 복부의 부위별 촬영조건에 따라 Rando phantom 에 $0^{\circ}$, $90^{\circ}$, $180^{\circ}$, $270^{\circ}$, 중심부에 각각 3개씩의 유리선량계를 부착하여 Field size $26.6{\times}20$, $15{\times}15$로 나누어 측정하였다. 또한 같은 방법으로 CBCT width를 16cm, 10cm로 나누어 동일하게 측정하였다. 결 과 : 2차원영상 AP 촬영은 입사방향인 $0^{\circ}$에서 가장 크게 측정되었으며 Field size 를 $26.6{\times}20$, $15{\times}15$로 변화 시켰을 때 흡수선량은 두부에서 각각 $1.44{\pm}0.26mGy$, $1.17{\pm}0.02mGy$, 흉부는 $3.08{\pm}0.86mGy$, $0.57{\pm}0.02mGy$, 복부는 $8.19{\pm}0.54mGy$ $4.19{\pm}0.08mGy$로 Field size 축소에 따라 평균 5~12%감소하였다. Lat 촬영 시에는 각각 5~8%감소하였다. 3차원영상 CBCT 에서는 width를 16 cm, 10 cm로 변화시킴에 따라 CBDI 측정값은 두부 $4.39{\pm}0.11mGy$, $3.99{\pm}0.13mGy$, 흉부(LDCT) $34.88{\pm}0.93(10.48{\pm}0.09)mGy$, $31.01{\pm}0.3(9.30{\pm}0.09)mGy$ 복부 $35.99{\pm}1.86mGy$, $32.27{\pm}1.35mGy$로 약 8~11%감소하였다. 결 론 : 2D는 조사면 크기를 줄여 5~12%, 3D는 width를 줄여줌으로써 8~11% 환자피폭선량을 감소시킬 수 있었다. 영상선량을 줄이기 위한 방사선사의 인식의 전환이 필요하고 다수의 CBCT 촬영시 치료처방선량에 영상선량의 포함여부도 고려되어야 할 것으로 사료된다.