• Nutrition Research and Practice
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• 제12권1호
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• pp.41-46
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• 2018

BACKGROUND/OBJECTIVES: Exposure of the normal lung tissue around the cancerous tumor during radiotherapy causes serious side effects such as pneumonitis and pulmonary fibrosis. Radioprotectors used during cancer radiotherapy could protect the patient from side effects induced by radiation injury of the normal tissue. Delphinidin has strong antioxidant properties, and it works as the driving force of a radioprotective effect by scavenging radiation-induced reactive oxygen species (ROS). However, no studies have been conducted on the radioprotective effect of delphinidin against high linear energy transfer radiation. Therefore, this study was undertaken to evaluate the radioprotective effects of delphinidin on human lung cells against a proton beam. MATERIALS/METHODS: Normal human lung cells (HEL 299 cells) were used for in vitro experiments. The 3-[4,5-dimethylthiazol-2-yl]-2,5 diphenyl tetrazolium bromide (MTT) assay assessed the cytotoxicity of delphinidin and cell viability. The expression of radiation induced cellular ROS was measured by the 2'-7'-dicholordihydrofluorescein diacetate assay. Superoxide dismutase activity assay and catalase activity assay were used for evaluating the activity of corresponding enzymes. In addition, radioprotective effects on DNA damage-induced cellular apoptosis were evaluated by Western blot assay. RESULTS: Experimental analysis, including cell survival assay, MTT assay, and Western blot assay, revealed the radioprotective effects of delphinidin. These include restoring the activities of antioxidant enzymes of damaged cells, increase in the levels of pro-survival protein, and decrease of pro-apoptosis proteins. The results from different experiments were compatible with each to provide a substantial conclusion. CONCLUSION: Low concentration ($2.5{\mu}M/mL$) of delphinidin administration prior to radiation exposure was radioprotective against a low dose of proton beam exposure. Hence, delphinidin is a promising shielding agent against radiation, protecting the normal tissues around a cancerous tumor, which are unintentionally exposed to low doses of radiation during proton therapy.

• 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.

• 한국진공학회지
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• 제22권6호
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• pp.341-347
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• 2013

동시 계수 도플러 넓어짐 양전자 소멸 분광법으로 n형과 p형 실리콘 시료에 40.0, 3.98 MeV 에너지를 가진 $0.0{\sim}20.0{\times}10^{13}protons/cm^2$ 양성자 빔 조사에 의한 결함을 측정하여 시료 특성을 조사하였다. 양전자와 전자의 쌍소멸로 발생하는 감마선 스펙트럼의 전자 밀도 에너지에 의한 수리적 해석 방법인 S-변수를 사용하여, 시료의 구조 변화를 측정하였다. 본 연구에서 측정된 S-변수는 시료에 조사된 양성자 조사량의 변화에 따라 결함이 증가하였으며, 그리고 40 MeV 양성자 빔의 세기는 n형 실리콘에서 빔의 조사량 $20.0{\times}10^{13}protons/cm^2$에서 3.98 MeV 보다 결함의 영향이 더 큰 것으로 나타났다. 그 결과 조사에 너지와 조사량의 상관관계를 비교 분석하였다. SRIM 시뮬레이션의 결과는, 양성자의 Bragg 피크 특성 때문에 시료 전체에 대한 결함으로 나타나기 보다는 양성자가 시료의 특정 깊이에 주로 결함을 형성하는 것을 보여 준다.

• 한국의학물리학회지:의학물리
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• 제27권4호
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• pp.267-271
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• 2016

In this study, we present the commissioning and validation results of a dedicated scanning nozzle. The dedicated scanning nozzle is installed in one of the two gantry treatment rooms at Samsung Proton Therapy Center. Following a successful completion of the acceptance test, the commissioning process including the beam data measurement for treatment planning system has been conducted. Extended measurements have been conducted as a validation of the clinical performance of the nozzle and various quality assurance protocols have been prepared.

• 한국의학물리학회지:의학물리
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• 제20권2호
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• pp.97-105
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• 2009

물 흡수선량표준을 기반으로 하는 선량측정 프로토콜에서는 전자선의 선질결정 지표는 $R_{50}$이며, 선량측정의 정확성을 향상시키기 위하여 전자선의 기준 에너지가 $R_{50}$>7 $g/cm^2$ (E${\gtrsim}$16 MeV)인 고에너지 전자선에서 표준기관에 소급성이 있는 원통형이온함의 물흡수선량교정계수을 이용한 평행평판형이온함의 교차교정을 권고하고 있다. 그러나 이러한 조건을 만족하는 고에너지 전자선은 모든 치료기관에서 보유하기가 어려운 실정이다. 따라서 본 연구에서는 평행평판형이온함의 교차교정 시 16 MeV 이상의 고 에너지 전자선뿐 아니라 12 MeV 이하의 전자선 에너지에서 얻은 평행평판형이온함의 교정계수를 이용하여 선량차이를 각각 비교하였다. 전자선 선량측정은 PTW 30013, Wellhofer FC65G의 Farmer형 원통형이온함과 PTW 34001, Wellhofer PPC40의 Roos형 평행평판형이온함을 이용하였으며 물팬텀내 기준깊이 $Z_{ret}=0.6R_{50}-0.1$(cm)에 원통형이온함과 평행평판형이온함을 같은 위치에 놓고 교차교정을 실시하였다. 교차교정 선질 20 MeV에서 결정된 교정계수를 적용한 물 흡수선량과 전자선에너지 12, 16 MeV에서의 물 흡수선량 차이는 0.2% 이내로 비교적 잘 일치하는 연구결과를 보였다. 그러므로 교차교정 선질 차이에 의한 흡수선량 값 상호 비교한 결과는 측정 불확도내에서 잘 일치하고 있어 각 기관에서 보유하고 있는 의료용가속기의 최고 전자선 선질에서의 교차교정도 유효하다고 사료된다.

• Applied Science and Convergence Technology
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• 제23권5호
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• pp.261-264
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• 2014

$SrTiO_3$ (STO) single crystal irradiated with a 3-MeV proton beam exhibits blue and green mixed luminescence. However, the same proton beam when used to irradiate STO with a very thin layer of deposited Pt does not show any luminescence. This Pt layer prevents any damage which may otherwise be caused by arcing, which stems from the accumulated surface voltage of tens of kV due to the charge induced by secondary electrons on the surface of the insulator during the ion beam irradiation process. Hence, the luminescence of ion-irradiated STO originates from the modification of the STO surface layer caused by arcing rather than from any direct ion beam irradiation effect. STO treated with atmospheric-pressure plasma, a simple and cost-effective method, also exhibits the same type of blue and green mixed luminescence as STO treated with an ion beam, as the plasma also creates a layer of surface damage due to arcing.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.192-194
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• 2002

We present the results on the calibration of iso-center positions using the quality assurance system established at PMRC for determination of center position in X-ray and proton irradiation fields. Details on the system are presented in another presentation in this session. The equipment in the system is mounted on a patient treatment bed in each proton exposure room, G1 or G2. A center of a stainless ball on the equipment is set at a cross of laser markers located around the iso-center and fixed on the room and on the snout in the gantry. A proton beam or an X-ray beam is exposed onto the ball through a brass collimator of 100 mm ${\times}$ 100 mm and projected onto the imaging plate set at I cm behind the ball. On the axis perpendicular to the thrust axis of the gantry on the imaging plate, a distance between a center of the collimator image and a center of the ball image varies as a cosine function of gantry angles unless the ball is set on the iso-center. An amplitude of the cosine curve shows the distance between the ball and the iso-center, an offset the offset of the collimator, and a phase shift at a zero crossing point the ball direction viewed from the iso-center. We present the relation among the iso-center position, the laser maker position, and the center of proton and X-ray irradiation fields. Its stability and its reproducibility are discussed.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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• pp.262-262
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• 2012

A multi-purpose cyclotron, MC50 has been operated to provide multi-ions of proton, deuteron and alpha at Korea Institute of Radiological and Medical Sciences (KIRAMS). Neutron is also produced through the (p,n) nuclear process with a Be target. However, a wide spectrum of current of ions is requested by beam users for carrying their various application fields. Therefore a simulation study is requested on the design of an axial injection system for high current proton and alpha beam extraction for radio-isotope productions and scientific researches. The purpose of this study is seeking a relatively simple method for the MC50 having higher alpha beam capability and also improving proton and deuteron beams currently used. We are considering two possibilities to improve the internal ion source and to install a new external axial injection system. The external injection system will be consisted of an Einzel lens, a steering magnet, a buncher, and a glazer lens placed in front of an inflector, which is located at the center of the main magnet.

• 대한방사선치료학회지
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• 제22권1호
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• pp.47-51
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• 2010

목 적: 고 에너지 양성자치료에 있어서 Air gap (환자와 Beam 사출구 사이의 거리)의 변화는 Lateral Penumbra의 증가로 불필요한 조사야를 형성할 수 있고, 치료부위에서 최대선량 증가와 최소선량 감소로 선량분포의 균질성을 저하시킬 수 있다. 이에 Air gap 변화에 따른 선량분포에 대해 비교, 연구해 보고자 한다. 대상 및 방법: 본원에서 양성자치료를 받은 Lung, Liver 환자 6명을 선정하여 크기가 다른 조사야 A와 조사야 B에서 Air gap을 2, 4, 6, 8, 10 cm로 설정하여 Proton external beam planning system을 통해 치료계획을 세웠다. Air gap에 따른 Lateral Penumbra 영역 및 DVH (Dose Volume Histogram)를 비교하고 PCTV영역의 최대선량 및 최소선량 값을 비교하였다. 또한 PCTV내에 선량의 균질성을 알기 위하여 Homogeneity index값을 비교, 분석하였다. 결 과: 각각의 조사야에서 Air gap의 변화(2, 4, 6, 8, 10 cm)에 따른 Lateral Penumbra영역을 분석한 결과 조사야 A에서 Air gap 2~10 cm변화에 따라 평균 1.36~1.75 cm까지 약 28.7%가 지속적으로 증가하였고 조사야 B에서 평균 1.36~1.79 cm까지 약 31.6%가 지속적으로 증가하였다. DVH를 분석한 결과 최대선량의 상대선량 백분율은 Air gap 2~10 cm일 때 평균 108.1%에서 평균 110.3%까지 약 2.03%가 지속적으로 증가하였고 최소선량의 상대선량 백분율은 평균 93.9%에서 평균 90.8%까지 약 3.31%가 지속적으로 감소하였다. Homogeneity index값은 평균 Air gap 2~10 cm까지 1.09~2.6으로 2배 이상 증가하였다. 결 론: 양성자 치료에 있어서 Air gap이 증가함에 따라 Lateral Penumbra 영역이 증가함을 알 수 있었고, 치료부위에서 최대선량 값의 증가와 최소선량 값의 감소로 인하여 Homogeneity index값이 증가함으로써 PCTV내에 Beam의 균질성이 떨어지는 것을 알 수 있었다. 이에 추후 양성자치료시 Air gap을 줄이기 위한 노력이 필요할 것으로 사료된다.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.214-215
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• 2002

Generally uniform dose distribution is assumed to be formed in a target region when a conventional dose formation method using a broad proton beam, a fixed modulation technique, a bolus and an aperture is employed. However, actual situations differ. We usually find non-uniformity in the target region. This is due to the insertion of a range-compensating bolus before the patient. Since the range-compensating bolus has an irregular shape, the scattering in the bolus depends on the lateral position. Dose distribution is overlapping results of dose distribution of pencil-proton beams traversing different lateral positions of the bolus. The lateral extent of dose distribution of each pencil beam traversing the different position differs each other at the same depth in the target object. This is a cause of the non-uniformity of the dose distribution. Therefore the same lateral extent of dose distribution should be attained for different pencil beams at the same depth to obtain a uniform dose distribution. For that purpose, we propose here a bi-material bolus. The bi-material bolus consists of a low-Z material determining mainly the range loss and a high-Z material defining mainly the scattering in the bolus. After passing through the bi-material bolus, protons traversing different lateral positions will have different residual range yet with the same lateral spread at a certain depth. Using the optimized bi-material bolus, we can obtain a more uniform dose distribution in the target region as expected.