• Nuclear Engineering and Technology
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• 제52권10호
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• pp.2410-2414
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• 2020

Heavy ions have a high potential for destroying deep tumors that carry the highest dose at the peak of Bragg. The peak caused by a single-energy carbon beam is too narrow, which requires special measures for improvement. Here, carbon-12 (¹²C) ion with different energies has been used as a source for calculating the dose distribution in the water phantom, soft tissue and bone by the code of Monte Carlobased FLUKA code. By increasing the energy of the initial beam, the amount of absorbed dose at Bragg peak in all three targets decreased, but the trend for this reduction was less severe in bone. While the maximum absorbed dose per bone-mass unit in energy of 200 MeV/u was about 30% less than the maximum absorbed dose per unit mass of water or soft tissue, it was merely 2.4% less than soft tissue in 400 MeV/u. The simulation result showed a good agreement with experimental data at GSI Darmstadt facility of biophysics group by 0.15 cm average accuracy in Bragg peak positioning. From 200 to 400 MeV/u incident energy, the Bragg peak location increased about 18 cm in soft tissue. Correspondingly, the bone and soft tissue revealed a reduction dose ratio by 2.9 and 1.9. Induced neutrons did not contribute more than 1.8% to the total energy deposited in the water phantom. Also during ¹²C ion bombardment, secondary fragments showed 76% and 24% of primary 200 and 400 MeV/u, respectively, were present at the Bragg-peak position. The combined treatment of carbon ions with neutron or electron beams may be more effective in local dose delivery and also treating malignant tumors.

• 한국정보통신학회:학술대회논문집
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• 한국정보통신학회 2013년도 춘계학술대회
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• pp.1020-1022
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• 2013

본 논문에서는 펄스방사선 선량 측정을 위한 Peak Detector를 설계하였다. 펄스방사선은 수ns ~ 수십ns의 초고속의 신호로 Peak 값을 측정하기 어렵다. Peak Detector는 센서에서 발생한 Peak 전압을 수ms 동안 유지하므로 ADC를 이용하여 데이터를 쉽게 측정할 수 있다. Peak Detector 시뮬레이션 결과 Peak 값을 1ms 이상 유지하는 것을 확인하였으며 펄스방사선 조사시험 결과 $1.95{\times}10^6rad/s$의 선량을 확인하였다.

• 방사성폐기물학회지
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• 제7권3호
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• pp.183-190
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• 2009

고준위폐기물 처분장의 기본적인 기능은 단기간에 과도한 방사성핵종이 유출되는 것을 방지하는데 있다. 이를 위해서는, 처분시스템의 구성요소들과 관련된 많은 기술 기준이 개발되고 수립되어야 한다. 처분장 안전성평가는 합리적으로 단순화된 모델에 바탕을 두고 처분장의 미래 전개에 대한 정량적인 결과를 산출하므로 안전성평가는 기술기준의 하나로 간주되고 있다. 본문에서는 평가기간, 선량 제한치 및 평가의 불확실성 등을 중심으로 안전성평가와 관련된 주요국의 기술기준을 조사하였다. 특히, 미국의 기준을 조사하는 과정에서 안전성평가에서 도출된 peak dose가 선량 제한치를 충족하지 못하는 경우, 평가기간 및 peak dose에 대한 미국 규제당국의 접근방안은 참고할만한 가치가 있음을 알 수 있었다.

• 한국진공학회지
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• 제9권3호
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• pp.216-220
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• 2000

실리콘이온 주입 후 $1100^{\circ}C$에서 열처리된 실리콘 산화막에서 Si+ dose 량의 변화에 대한 광루미니센스의 변화를 관찰하였다. 모든 시료에서 가시광과 적외선영역의 광루미니센스를 관찰할 수 있었다. 광루미니센스의 peak는 7000 $\AA$, 7400 $\AA$, 그리고 8400 $\AA$ 근처에 있었으며, $Si^+$ dose량이 변함에 따라 peak의 위치와 강도가 변하였다. 이온 주입되는 $Si^+$ dose량이 $1\times10^{17}\textrm{cm}^2$일 때 광루미니센스에서 특이하게 3개의 peak를 가지고 있었으며 다른 $Si^+$ dose량의 시료에 비하여 큰 강도를 보여준다. 주입된 $Si^+$ 이온들이 실리콘 산화막내에 서 결함을 생성하여서 광루미니센스에 기여를 한다. $Si^+$ dose량과 열처리 시간 등을 변화시키면 높은 에너지의 Si 위주 radiative defect, 낮은 에너지의 Si 위주 radiative defect, 그리고 nonradiative defect들이 관계하는 것으로 생각되어져 왔으나 적절한 $Si^+$ dose량으로 더 많은 radiative defect를 생성시킬 수 있음을 확인하였다. $Si^+$ dose량을 조절함으로서 광루미니센스의 peak의 위치와 강도를 제어할 수 있을 것이다.

• 한국방사선학회논문지
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• 제13권2호
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• pp.253-260
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• 2019

방사선 선량 증강은 물질과의 상호작용 단면적을 높여 국소 부위에 대한 선량을 증가시키는 방법으로 선에너지부여 및 상대적 생물학적 효과비 증가로 치료가능비 향상에 기여할 수 있다. 선량 증강에 대한 선행 연구는 X, ${\gamma}$선에 대한 보고가 주를 이루고 있으나, 본 연구에서는 MCNP6를 이용한 몬테칼로 시뮬레이션을 바탕으로 양성자 선원에 대해 선량 증강 현상을 분석하였다. 수학적 모델 방법에 따라 확산된 피크의 양성자 선원에 대한 에너지 분포와 상대적 강도를 산출하였으며, 금, 아이오딘, 가돌리늄의 선량 증강 물질에 대한 선량증강비와 깊이 변화에 따른 에너지 분포를 평가하였다. 금을 이용한 증강 현상에서 1.085-1.120배, 가돌리늄에서는 1.047-1.091배의 선량증강비를 나타내었다. 또한 깊이에 따른 흡수에너지 변화로 인해 실질 비정과 95% 선량 구간의 감소를 나타내었으며, 이는 선량 증강 현상과 더불어 종양조직에 불확실한 선량 전달로 이어질 수 있으므로 증강 물질의 질량 저지능으로부터 확산된 피크 구간의 적절한 보정이 필요할 것으로 사료된다. 본 연구에서 모의모사를 통한 선량 증강 현상의 분석은 실질적인 증강 효과 확인을 위한 체내 외 실험의 기초자료로써 활용될 것으로 기대한다.

• 한국의학물리학회지:의학물리
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• 제31권4호
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• pp.135-144
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• 2020

Purpose: Gafchromic films for proton dosimetry are dependent on linear energy transfers (LETs), resulting in dose underestimation for high LETs. Despite efforts to resolve this problem for single-energy beams, there remains a need to do so for multi-energy beams. Here, a bimolecular reaction model was applied to correct the under-response of spread-out Bragg peaks (SOBPs). Methods: For depth-dose measurements, a Gafchromic EBT3 film was positioned in water perpendicular to the ground. The gantry was rotated at 15° to avoid disturbances in the beam path. A set of films was exposed to a uniformly scanned 112-MeV pristine proton beam with six different dose intensities, ranging from 0.373 to 4.865 Gy, at a 2-cm depth. Another set of films was irradiated with SOBPs with maximum energies of 110, 150, and 190 MeV having modulation widths of 5.39, 4.27, and 5.34 cm, respectively. The correction function was obtained using 150.8-MeV SOBP data. The LET of the SOBP was then analytically calculated. Finally, the model was validated for a uniform cubic dose distribution and compared with multilayered ionization chamber data. Results: The dose error in the plateau region was within 4% when normalized with the maximum dose. The discrepancy of the range was <1 mm for all measured energies. The highest errors occurred at 70 MeV owing to the steep gradient with the narrowest Bragg peak. Conclusions: With bimolecular model-based correction, an EBT3 film can be used to accurately verify the depth dose of scanned proton beams and could potentially be used to evaluate the depth-dose distribution for patient plans.

• 대한임상독성학회지
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• 제7권2호
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• pp.156-163
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• 2009

Purpose: Doxylamine succinate (DS) is frequently used to treat insomnia and it may induce rhabdomyolysis in the overdose cases. The purpose of this study is to evaluate the factors that can predict the serum creatine kinase (CK) level normalization time for patients with rhabdomyolysis due to DS ingestion. Methods: This study was conducted on 71 patients who were admitted with rhabdomyolysis after DS ingestion during the period from January 2000 to July 2009. Rhabdomyolysis was defined as a serum CK level over 1,000 U/L. The collected data included the general characteristics, the anticholinergic symptoms, the ingested dose, the peak serum CK level, the time interval (TI) from the event to the peak CK level and the TI from the event to a CK level below 1,000 U/L. We evaluated the correlation between the patients' variables and the TI from the event to the peak CK level time and the time for a CK level below 1,000 U/L. Results: The mean ingested dose per body weight (BW) was $30.86{\pm}18.63\;mg/kg$ and the mean TI from the event to treatment was $4.04{\pm}3.67$ hours. The TI from the event to the peak CK level was longer for the patients with a larger ingestion dose per BW (r=0.587, p<0.05). The CK normalization time was longer for the patients with a larger ingested dose per BW (r=0.446, p<0.05) and a higher peak CK level (r=0.634, p<0.05). Conclusion: The ingested dose per BW was correlated with the TI from the event to the peak CK level, and the ingested dose per BW and the peak CK level have significant correlations with the CK normalization time. These factors may be used to determine the discharge period of patients who had rhabdomyolysis following a OS overdose.

• 한국안전학회지
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• 제9권1호
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• pp.48-55
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• 1994

In this paper, It is studied that the variation of the dielectric absorption of the specimen according to the change with $^{60}$ Co-${\gamma}$ ray irradiation dose of the influence of temperature and applied voltage. In order to investigate the effect of irradiated oriented polypropylene film, we have observed dielectric properties within the temporature range of 30~130 ($^{\circ}C$) and voltage range of 100~250 (V). As for the dependency of temperature by tan $\delta$, the $\alpha$ peak which appears at high temperature increases accordingly to the increment of irradiation dose which is contributed by the crystal region and moves towards the high temperature. The $\beta$ peak which appears the orientation by dipoles and molecular motions in the amorphous region at low temperature. For the dependency of voltage by tan $\delta$ at low temperature, the peak of the tan $\delta$ shifts accordingly to the increment of irradiation dose towards the high temperature region.

• Nuclear Engineering and Technology
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• 제53권8호
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• pp.2767-2773
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• 2021

We used the GEANT4 Monte Carlo MC Toolkit to simulate carbon ion beams incident on water, tissue, and bone, taking into account nuclear fragmentation reactions. Upon increasing the energy of the primary beam, the position of the Bragg-Peak transfers to a location deeper inside the phantom. For different materials, the peak is located at a shallower depth along the beam direction and becomes sharper with increasing electron density NZ. Subsequently, the generated depth dose of the Bragg curve is then benchmarked with experimental data from GSI in Germany. The results exhibit a reasonable correlation with GSI experimental data with an accuracy of between 0.02 and 0.08 cm, thus establishing the basis to adopt MC in heavy-ion treatment planning. The Kolmogorov-Smirnov K-S test further ascertained from a statistical point of view that the simulation data matched the experimentally measured data very well. The two-dimensional isodose contours at the entrance were compared to those around the peak position and in the tail region beyond the peak, showing that bone produces more dose, in comparison to both water and tissue, due to secondary doses. In the water, the results show that the maximum energy deposited per fragment is mainly attributed to secondary carbon ions, followed by secondary boron and beryllium. Furthermore, the number of protons produced is the highest, thus making the maximum contribution to the total dose deposition in the tail region. Finally, the associated spectra of neutrons and photons were analyzed. The mean neutron energy value was found to be 16.29 MeV, and 1.03 MeV for the secondary gamma. However, the neutron dose was found to be negligible as compared to the total dose due to their longer range.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1993년도 추계학술대회 논문집
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• pp.80-84
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• 1993

In this research, we studied the variation of the dielectric loss absorption of the dielectric loss absorption of the sample according with the change to $\^$60/Co-${\gamma}$-ray irradiation dose of the influence of temperature and applied voltage. In order to investigate the effect of irradiation oriented polypropylene film, we have observed dissipation factor within the temperature range of 30∼130 [$^{\circ}C$] and voltage range of 100∼250$^{\circ}C$ [V]. As for the dependency of temperature by dissipation factor, the ${\alpha}$-peak which appears at high temperature increases accordingly to the increasement of irradiation dose which is contributed by the crystal region and moves towards the high temperature. The ${\beta}$-peak which appears at low temperature is origined from dipoles and molecular motions in the amorphous region. As for the dependency of voltage by tan$\delta$, at low temperature the peak of the tan$\delta$, at low temperature the peak of the tan$\delta$ shifts accordingly to the increasement of irradiation dose towards the high temperature region.