• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.260-262
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• 2002

An accurate measurement of dose distribution is indispensable to perform radiation therapy planning. A measurement technique using a radiographic film, which is called a film dosimetry, is widely used because it is easy to obtain a dose distribution with a good special resolution. In this study, we tried to develop an analyzing system for the film dosimetry using usual office automation equipments such as a personal computer and an image scanner. A film was sandwiched between two solid water phantom blocks (30 ${\times}$ 30 ${\times}$ 15cm). The film was exposed with Cobalt-60 ${\gamma}$-ray whose beam axis was parallel to the film surface. The density distribution on the exposed film was stored in a personal computer through an image scanner (8bits) and the film density was shown as the digital value with NIH-image software. Isodose curves were obtained from the relationship between the digital value and the absorbed dose calculated from percentage depth dose and absorbed dose at the reference point. The isodose curves were also obtained using an Isodose plotter, for reference. The measurements were carried out for 31cGy (exposure time: 120seconds) and 80cGy (exposure time: 300seconds) at the reference point. While the isodose curves obtained with our system were drawn up to 60% dose range for the case of 80cGy, the isodose curves could be drawn up to 80% dose range for the case of 31cGy. Furthermore, the isodose curves almost agreed with that obtained with the isodose plotter in low dose range. However, further improvement of our system is necessary in high dose range.

• 센서학회지
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• 제23권3호
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• pp.197-201
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• 2014

TEPC (Tissue Equivalent Proportional Counter) was usually used for high LET radiation dosimetry. We developed a prototype TEPC for micro-dosimetry in the range of $0.2{\sim}300 keV/{\mu}m$. And, the simulated site diameter of the TEPC is $2{\mu}m$, of similar size to a cell nucleus. For purposes of characterization the response for high LET radiation of the TEPC has been investigated under 135MeV/u Carbon ions in HIMAC (Heavy Ion Medical Accelerator). We determined the gas multiplication factor and measured the lineal energy spectrum [yd(y)] of 135 MeV/u Carbon ions. The value of the gas multiplication factor was 315 at 700 V bias voltage. As a result of the experiment, we could more understand the performance of the TEPC for high LET (Linear Energy Transfer) radiation. And the procedure of high LET radiation dosimetry using TEPC is established.

• Journal of the Korean Physical Society
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• 제73권10호
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• pp.1571-1576
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• 2018

We developed and evaluated an algorithm to calculate the target radiation dose in cancer patients by measuring the transmitted dose during 3D conformal radiation treatment (3D-CRT) treatment. The patient target doses were calculated from the transit dose, which was measured using a glass dosimeter positioned 150 cm from the source. The accuracy of the transit dose algorithm was evaluated using a solid water phantom for five patient treatment plans. We performed transit dose-based patient dose verification during the actual treatment of 34 patients who underwent 3D-CRT. These included 17 patients with breast cancer, 11 with pelvic cancer, and 6 with other cancers. In the solid water phantom study, the difference between the transit dosimetry algorithm with the treatment planning system (TPS) and the measurement was $-0.10{\pm}1.93%$. In the clinical study, this difference was $0.94{\pm}4.13%$ for the patients with 17 breast cancers, $-0.11{\pm}3.50%$ for the eight with rectal cancer, $0.51{\pm}5.10%$ for the four with bone cancer, and $0.91{\pm}3.69%$ for the other five. These results suggest that transit-dosimetry-based in-room patient dose verification is a useful application for 3D-CRT. We expect that this technique will be widely applicable for patient safety in the treatment room through improvements in the transit dosimetry algorithm for complicated treatment techniques (including intensity modulated radiation therapy (IMRT) or volumetric modulated arc therapy (VMAT).

• Nuclear Engineering and Technology
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• 제42권6호
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• pp.670-679
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• 2010

In this paper, a new approach using a pixel-based correction method was developed to fix the non-uniform responses of flat-bed type scanners used for radiochromic film dosimetry. In order to validate the method's performance, two cases were tested: the first consisted of simple dose distributions delivered by a single port; the second was a complicated dose distribution composed of multiple beams. In the case of the simple individual dose condition, ten different doses, from 8.3 cGy to 307.1 cGy, were measured, horizontal profiles were analyzed using the pixel-based correcton method and compared with results measured by an ionization chamber and results corrected using the existing correction method. A complicated inverse pyramid dose distribution was made by piling up four different field shapes, which were measured with GAFCHROMIC$^{(R)}$EBT film and compared with the Monte Carlo calculation; as well as the dose distribution corrected using a conventional method. The results showed that a pixel-based correction method reduced dose difference from the reference measurement down to 1% in the flat dose distribution region or 2 mm in a steep dose gradient region compared to the reference data, which were ionization chamber measurement data for simple cases and the MC computed data for the complicated case, with an exception for very low doses of less than about 10 cGy in the simple case. Therefore, the pixel-based scanner correction method is expected to enhance the accuracy of GAFCHROMIC$^{(R)}$EBT film dosimetry, which is a widely used tool for two-dimensional dosimetry.

• Journal of Radiation Protection and Research
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• 제27권1호
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• pp.37-49
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• 2002

방사선치료 시 종양에 정확한 양의 방사선을 조사하는 것은 국소 재발을 방지하고 합병증의 빈도를 낮춰 효과적인 치료를 가능하게 하는 중요한 요소이다. 종양에 조사되는 방사선량의 측정을 통해 치료의 정확성을 확인하기 위한 여러 방법들이 시도되고 있으며, 투과선량을 이용한 측정법도 그 중 한 예로 비침습적이며 매 치료 시 측정이 가능한 장점을 가지고 있다. 본 교실에서는 투과선량을 이용한 in vivo 선량측정시스템과 임의의 치료 조건에서 투과선량을 계산하기 위한 알고리즘을 개발하였다. 본 교실에서 개발한 in vivo 선량측정시스템의 단기간 및 장기간의 재현성을 확인하고, 환자의 방사선치료에서의 이용 시 발생할 수 있는 문제점을 파악하고 알고리즘의 정확성을 확인하기 위하여 본 연구를 시행하였다. 2000년 7월 25일부터 8월 14일 사이에 방사선치료를 시행 받은 환자 66명을 대상으로 투과선량의 측정을 시행하였으며, 이 중 골반부위의 방사선 치료를 3회 이상 시행 받은 11명의 환자를 대상으로 측정선량과 예측선량의 비교 분석을 시행하였다. 측정시스템의 재현성의 확인을 위하여 환자의 치료 전 및 치료 중 매시간 기준 조사조건에서 측정치를 확인하였다. 일별 및 일 중 변동은 ${\pm}2%$ 이내로 재현성을 확인할 수 있었다. 본 시스템의 사용 시 별다른 문제점은 없었으나, 2명의 흉부 치료환자에서 투과선이 치료용테이블의 측면 금속을 관통하는 문제가 발생하였다. 골반부위 환자에서는 골반부위의 불균질조직에 의한 영향의 확인을 위하여, CT 및 simulation film을 이용하여 골 조직의 두께를 확인하여 보정 전 및 후의 값을 비교하였다. 전후방 및 후방조사야의 경우 골 조직의 보정을 시행하지 않은 경우 평균오차가 -5.20% 내지 +2.20%이었으며, 보정을 시행한 경우 -0.62%내지 +3.32%로 환자에 따라 정도의 차이는 있으나 골 보정이 필요함을 확인할 순 있었다. 측정치와 예측치 간 오차의 표준편차는 1.19%내지 2.46%로서 재현성이 높음을 확인할 수 있었다. 좌우 측방조사야에서 골 보정을 시행하지 않은 경우 평균오차는 -10.80%내지 +3.46%로서 골 조직의 보정이 필요하지 않은 1인의 환자를 제외하면 모두 음수 값을 지녔고, 보정을 시행한 경우 -0.55% 내지 +3.50%의 평균오차를 지녀 골 보정의 필요성을 확인할 수 있었다. 측정치와 예측치 간 오차의 표준편차는 1.09%내지 6.98%로 전후방조사야의 경우보다 재현성이 낮음을 알 수 있었다. 복와위로 방사선치료를 시행 받은 환자의 경우를 제외하면, 표준편차는 1.09%내지 3.12%로 1례 외에는 2.57% 이내로 재현성이 높음을 확인할 수 있었다. 본 실험을 통하여 in vivo 선량측정시스템의 안전성과 재현성을 확인할 수 있었다. 정확한 예측치를 얻기 위하여 불균질 조직이 조사야에 포함되는 경우 보정이 요구되며, 골반의 경우 골 조직의 보정이 중요한 요인임을 알 수 있었다. 이를 위하여 불균질 조직에 대한 정확한 정보가 요구되며, 이는 CT 영상을 이용하는 것이 크게 도움이 되리라 생각된다.

• 대한방사선치료학회지
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• 제16권1호
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• pp.29-37
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• 2004

목적 : 자궁경부암 환자의 고선량률 근접치료 시 부작용을 줄이기 위해 가장 주의 깊게 선량을 고려해야 할 곳은 직장과 방광이다. 일반적으로 직장이나 방광에서의 선량값은 Planning장치의 계산값에만 의존하고 있는 상태이고, TLD를 이용한 직장 선량분석은 보고된 바 있으나 In vivo dosimetry(Diode detector)를 이용한 보고는 거의 없었다. 본 연구에서는 자궁경부암 환자치료 시 매번 diode detector를 직장 내에 삽입하여 직장 선량을 측정하고 측정된 값을 토대로 직장의 부작용을 줄이는데 기초 자료로 활용 하고자 하였다. 대상 및 방법 : 2003년 2월부터 2003년 6월까지 Ir-192 동위원소 고선량률 근접치료기로 치료받은 자궁경부암환자 6명(tandem and ovoid 4명, cylinder 1명, tandem and cylinder 1명)을 대상으로 총 28회 측정을 실시하였고 직장내 Diode detector를 매번 측정 시마다 anterior, lateral film을 동일한 지점에서 촬영 후, Planing을 실시하여 측정값과 비교해 보았다. 결과 : 4명의 tandem md ovoid에서 3명의 직장내 Diode detector측정값의 평균과 편차는 $274.1{\pm}13.4cGy$이고 1명의 tandem and ovoid에서 $126.1{\pm}7.2cGy$, cylinder에서 $99.7{\pm}7.1cGy$, tandem and cylinder에서 $77.7{\pm}11.5cGy$이었다. 결론 : 직장의 매 측정 시마다 Diode detector측정값은 직장의 상태에 따라 표준편차가 매우 크므로 단 한번의 치료계획 계산 값으로 직장의 부작용을 예측하는 것은 어렵다. 본 연구에서 얻어진 결과로 볼 때 가능하다면 TLD 또는 In vivo dosimetry 장비를 이용하여 치료 시마다 실측하여 직장의 부작용을 판단하는 것이 중요하며 직장의 부작용이 예상될 시 gauze packing 및 조사시간을 조절하거나 shielded된 기구를 사용하여 직장의 선량을 낮추도록 하는 것이 필요하다고 사료된다.

• Nuclear Medicine and Molecular Imaging
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• 제41권4호
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• pp.265-271
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• 2007

Radionuclide therapy has been an important field in nuclear medicine. In radionuclide therapy, relevant evaluation of Internally absorbed dose is essential for the achievement of efficient and sufficient treatment of incurable disease, and can be accomplish by means of accurate measurement of radioactivity in body and its changes with time. Recently, the advances of nuclear medicine imaging and multi modality imaging processing techniques can provide change of more accurate and easier measurement of the measures commented above, in cooperation of conventional imaging based approaches. in this review, basic concept for internal dosimetry using nuclear medicine imaging is summarized with several check points which should be considered In real practice.

• Nuclear Medicine and Molecular Imaging
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• 제43권4호
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• pp.259-279
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• 2009

Radioiodine ablation therapy has been considered to be a standard treatment for patient with differentiated thyroid cancer after total thyroidectomy. Patients may need to be hospitalized to reduce radiation exposure of other people and relatives from radioactive patients receiving radioiodine therapy. Medical staffs, nursing staffs and technologists sometimes hesitate to contact patients in radioiodine therapy ward. The purpose of this paper is to introduce radiation dosimetry, estimate radiation dose from patients and emphasize the safety of radiation exposure from patients treated with high dose radioiodine in therapy ward. The major component of radiation dose from patient is external exposure. However external radiation dose from these patients treated with typical therapeutic dose of 4 to 8 GBq have a very low risk of cancer induction compared with other various risks occurring in daily life. The typical annual radiation dose without shielding received by patient is estimated to be 5 to 10 mSv, which is comparable with 100 to 200 times effective dose received by chest PA examination. Therefore, when we should keep in mind the general principle of radiation protection, the risks of radiation exposure from patients are low and the medical personnel are considered to be safe from radiation exposure.

• Nuclear Engineering and Technology
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• 제6권1호
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• pp.3-8
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• 1974

천연 녹주석의 방사선조사에 의한 효과를 없애기 위한 열처리방법을 연구하였다. Glow곡선분석에서 최적열처리시간과 온도는 145$0^{\circ}C$에서 1시간이었고, 녹주석을 다시 사용할 시에는 145$0^{\circ}C$에서 1시간동안 열처리를 다시 할 필요는 없고 55$0^{\circ}C$에서 1시간만 열처리를 하면 된다. 145$0^{\circ}C$에서 열처리된 녹주석시료를 $^{60}$Co감마선으로 100R 조사한 후 glow곡선을 그려보니 $65^{\circ}C$와 20$0^{\circ}C$에서 glow peaks를 발견하였다. $65^{\circ}C$ glow peak는 곧 없어졌으나 20$0^{\circ}C$ glow peak는 매우 안정하였다. 따라서 열형광방사선측정에는 20$0^{\circ}C$ glow peak를 이용하여 $^{60}$Co감마선을 측정할 수 있다.

• Journal of Radiation Protection and Research
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• 제36권3호
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• pp.107-118
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• 2011

Conventional (SRS) and fractionated (FSRS) stereotactic radiosurgery necessarily require stringent overall target point accuracy and precision. We determine three-dimensional intracranial target point deviations (TPDs) in a whole treatment procedure using magnetic resonance image (MRI)-based polymer-gel dosimetry, and suggest a technique for overall system tests. TPDs were measured using a custom-made head phantom and gel dosimetry. We calculated TPDs using a treatment planning system. Then, we compared TPDs using mid bi-plane and three-dimensional volume methods with spherical and elliptical targets to determine their inherent analysis errors; finally, we analyzed regional TPDs using the latter method. Average and maximum additive errors for ellipses were 0.62 and 0.69 mm, respectively. Total displacements were 0.92 ${\pm}$ 0.25 and 0.77 ${\pm}$ 0.15 mm for virtual SRS and FSRS, respectively. Average TPDtotal at peripheral regions was greater than that at central regions for both. Overall system accuracy was similar to that reported previously. Our technique could be used as an overall system accuracy test that considers the real radiation field shape.