• 대한디지털의료영상학회논문지
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• 제13권1호
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• pp.7-11
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• 2011

As applications of radiation grow wider from use in the early detection of lesions and preventive diagnosis purposes to the treatment of diseases, the possibilities for patients and working professionals to be exposed to radiation are becoming greater than ever. This can not only directly bring about an increase in patient's individual radiation exposure, but also brings about an increase in the annual radiation dose of working professionals. Therefore, research and countermeasures to reduce radiation dosage are required. In this study, space dosimetry has been divided into two separate measuments with an understanding of the increasing number of angiography procedures: front perspective and side perspective. According to the results of the isodose curve, a way to minimize radiation exposure in working professionals has been suggested. This was made possible by workers through awareness of suitable working positions.

• Radiation Oncology Journal
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• 제11권2호
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• pp.421-430
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• 1993

The calculation of dose distribution in multiple arc stereotactic radiotherapy is a three-dimensional problem and, therefore, the three-dimensional dose calculation algorithm is important and the algorithm's accuracy and reliability should be confirmed experimentally. The aim of this study is to verify the dose distribution of stereotactic radiosurgery experimentally and to investigate the effect of the beam quality, the number of arcs of radiation, and the tertiary collimation on the resulting dose distribution. Film dosimetry with phantom measurements was done to get the three-dimensional orthogonal isodose distribution. All experiments were carried out with a 6 MV X-ray, except for the study of the effects of beam energy on dose distribution, which was done for X-ray energies of 6 and 15 MV. The irradiation technique was from 4 to 11 arcs at intervals of from 15 to 45 degrees between each arc with various field sizes with additional circular collimator. The dose distributions of square field with linear accelerator collimator compared with the dose distributions obtained using circular field with tertiary collimator. The parameters used for comparing the results were the shape of the isodose curve, dose fall-offs fom $90\%$ to $50\%$ and from $90\%\;to\;20\%$ isodose line for the steepest and shallowest profile, and $A=\frac{90\%\;isodose\;area}{50\%\;isodose\;area-90\%\;isodose\;area}$(modified from Chierego). This ratio may be considered as being proportional to the sparing of normal tissue around the target volume. The effect of beam energy in 6 and 15 MV X-ray indicated that the shapes of isodose curves were the same. The value of ratio A and the steepest and shallowest dose fall-offs for 6 MV X-ray was minimally better than that for 15 MV X-ray. These data illustrated that an increase in the dimensions of the field from 10 to 28 mm in diameter did not significantly change the isodose distribution. There was no significant difference in dose gradient and the shape of isodose curve regardless of the number of arcs for field sizes of 10, 21, and 32 mm in diameter. The shape of isodose curves was more circular in circular field and square in square field. And the dose gradient for the circular field was slightly better than that for the square field.

• Radiation Oncology Journal
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• 제2권1호
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• pp.101-106
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• 1984

Various methods are available for determination of exposure time in intracavitary radiotherapy of the carcinoma of the uterine cervix. To determine the accuracy of dose calculation with isodose curve for TAO applicator, comparison with results calculated by computer for radiotherapy treatment Planning was done in 24 procedures done in 12 consecutive patients with the carcinoma of the uterine cervix from May to December, 1983. The results are as follows: 1. The average dose rate Per hour of Point A was 87.70 rad, being 89.91 rad ana 85.49 rad in left and right, respectively. 2. The average percentage of dose rate of point A calculated by isodose curve method over that by computer was $101.28\%$ and the difference was less than $5\%$ in 17 Procedures and over $10\%$ in only 3 procedures. 3. The average percentage in case of point B was $108.67\%$. In conclusion, in most cases the difference was less than 200 rad for point A and less than 100 rad for point B during 2 courses of intracavitary radiotherapy. And so the dose rate calculation with isodose curve for TAO applicator is comparatively accurate.

• 대한의용생체공학회:의공학회지
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• 제34권2호
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• pp.73-79
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• 2013

Purpose: The purposes of this study were to measure the dose distribution of Photodynamic therapy(PDT) laser with 635 nm wavelength using GafChromic film. Method & Result: We made each output 300 J by changing mW and sec using the laser beam radiation mode such as C.W(Continuous Wave) mode, Pulse mode and Burst Pulse mode and measured the does at 0 mm and 5 mm of distance from optic fiber catheter end to the film, and at 5 mm distance by changing the angle of the end of the optic fiber catheter as $0^{\circ}$ and $0.5^{\circ}$. The radiated film was scanned and OD(Optical Density) was compared. And two-dimensional isodose curves were obtained and the consistency of shapes was compared. It was confirmed that there was consistency between optic density and the dose radiated on the film when we radiated GafChromic film by changing distance and angle of 300 J output in each radiation mode coordinating mW and sec. Conclusion: In this study, we could identify the stability according to changes in laser beam modes, changes in output according to distance, changes in uniformity according to angle, and beam profiles using GafChromic film, and we could also get two-dimensional isodose curve. It was found that small change in the distance and angle that is made when optic fiber catheter was contacted on the treatment area did not make big effects on the output of beam and the uniformity of dose, and it was also found that GafChromic film could be utilized for the purpose of QA of PDT laser beam.

• Asian Pacific Journal of Cancer Prevention
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• 제17권1호
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• pp.197-200
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• 2016

Background: Wedge filters are commonly used in radiation oncology for eliminating hot spots and creating a uniform dose distribution in optimizing isodose curves in the target volume for clinical aspects. These are some limited standard physical wedges ($15^{\circ}$, $30^{\circ}$, $45^{\circ}$, $60^{\circ}$),or creating an arbitrary wedge angle, like motorized wedge or dynamic wedge,${\ldots}$ The new formulation is presented by the combination of wedge fields for determining an arbitrary effective wedge angles. The isodose curves also are derived for these wedges. Materials and Methods: we performed the dosimetry of Varian Clinac 2100C/D with Scanditronix Wellhofer water blue phantom, CU500E, OmniPro - Accept software and 0.13cc ionization chamber for 6Mv photon beam in depth of 10cm (reference depth) for universal physical wedges ($15^{\circ}$, $30^{\circ}$, $45^{\circ}$, and $60^{\circ}$) and reference field $10.10cm^2$. By combining the isodose curve standard wedge fields with compatible weighting dose for each field, the effective isodose curve is calculated for any wedge angle. Results: The relation between a given effective wedge angle and the weighting of each combining wedge fields was derived. A good agreement was found between the measured and calculated wedge angles and the maximum deviation did not exceed $3^{\circ}$. The difference between the measured and calculated data decreased when the combined wedge angles were closer. The results are in agreement with the motorized single wedge appliance in the literature. Conclusions: This technique showed that the effective wedge angle that is obtained from this method is adequate for clinical applications and the motorized wedge formalism is a special case of this consideration.

• Radiation Oncology Journal
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• 제3권1호
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• pp.59-64
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• 1985

Computation of three dimensional dose distribution using CT image and RT plan was applied to a case of pituitary adenoma. Algorithm was based on two dimensional Tissue Maximun Ratio model extended to the third dimension. The resulting isodose curve of transeverse, coronal and sagittal section was demonstrated. This RT plan allows computation of dose distribution in any arbitarily defined plane in addition to conventional cross sectional view.

• 대한의용생체공학회:학술대회논문집
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• 대한의용생체공학회 1994년도 추계학술대회
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• pp.85-87
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• 1994

In this paper, we present an object-oriented stereotactic radiosurgery planning system, which accepts medical images such as CT and angiography, transforms the coordinates to a reference frame coordinate, calculates dose distributions, and finally displays isodose curves over the images. The user finds an adequate one for radiosurgeries after performing computer simulations on different treatment parameter sets. The object-oriented design concept was fully applied to the system composed of seven manager objects of different classes: a patient information manager, a user-interface manager, a coordinate transformation manager, a blackboard manager, a dose calculation manager, an isodose curve display manager, and a report manager. All the user interactions are carried out through the use of mouse buttons. The performance of the system was verified by four physicians and two medical physicists, and now is being used in two clinical sites.

• 대한방사선치료학회지
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• 제7권1호
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• pp.92-96
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• 1995

All patients who will Undergo irraidiation of the oral cavity cancer will need dental before and during Radiotherapy. The extent of the region and the presence of numerous critical normal tissues(mucosa, gingiva, teeth and the alveolar ridge, alveolar bony structure, etc) in the oral cavity area, injury to which could result in serious functional impairment. Therefore I evaluate the Usefulness of custom-made intraoral shielding device before and during Radiotherapy in oral cavity cancer. Materials and Methods(1) : Manufacture process of Custom-made intraoral shielding device Containing Cerroband. A. Acquisition of impression B. Matrix Constitution C. Separation by Separator D. Sprincle on method E. Trimming F. Spacing G. Fill with Cerroband Materials and Methods (2) A. Preannealing B. TLD Set up C. Annealing D. TLD Reading = Results = Therefore dosimetric characteristics in oral cavity by TLD Compared to isodose curve dose distribution Ipsilateral oral mucosa, Contralateral oral mucosa, alveolar ridge, tongue, dose was reduced by intraoral shielding device containning Cerroband technique Compard to isodose plan = Conclusions = The custom-made intra-oral shielding device containing Cerroband was useful in reducing the Contralateral oral mucosa dose and Volume irradiated.

• Radiation Oncology Journal
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• 제25권4호
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• pp.268-277
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• 2007

목적: 호흡에 의한 종양의 움직임은 사이버나이프를 이용한 정위적 방사선수술과 같은 정확한 치료에 있어 고려할 만한 방해 요인이다 이 연구에서는 사이버나이프를 이용한 방사선 수술의 Interplay현상을 보고자 팬텀을 움직이게 하고 또한 움직이지 않게 하여 선량 분포의 왜곡을 조사하였다. 대상 및 방법: 팬텀은 $2.5{\times}2.5{\times}5.0$ 인치의 4개의 직육면체로 구성된 폴리에틸렌과 2장의 Gafchromic 필름으로 구성되었다. 치료 계획은 20, 30, 40, 50 mm지름을 가진 구를 가상하여 사이버나이프 치료기를 이용하여 104개의 빔 방향과 single center mode의 치료 계획 하에 총 30 Gy를 조사하였다. 특별히 제작된 로봇은 팬텀을 좌우, 전후, 두미쪽으로 각각 5, 10, 20 mm 움직이도록 고안되었다. 필름의 optical density을 이용하여 정적인 상태의 팬텀과 로봇에 의해 움직일 때의 팬텀의 선량 분포를 구하였다. 결 과: 정적인 상태에서 종양을 모두 포함할 수 있는 최소의 등선량은 20 mm 종양의 경우 80%, 30 mm에 84%, 40 mm에 83%이며 50 mm 종양에 80%였다. 정적인 상태와 움직일 때의 팬텀 사이에서 발생한 선량 분포의 차이(gap)는 20 mm 종양에서 두미방향으로 각각 3.2, 3.3 cm이며 오른쪽 3.5 mm, 왼쪽 1.1 mm였다. 30 mm 종양의 경우는 각각 3.9, 4.2, 2.8과 0 mm였고 40 mm 종양은 각각 4.0, 4.8, 1.1, 0 mm였다. 50 mm 종양의 경우 각각 3.9, 3.9, 0.0 mm였다. 결 론: 20 mm의 적은 종양을 치료할 때 80%의 등선량이 계획되더라도 움직이는 실제 치료에 있어 종양 움직임을 보완하기 위하여 60% 등선량으로 처방할 필요가 있다. 이때 두 등선량 곡선의 차이는 5 mm정도이다. 또한 30, 40과 50 mm의 종양에서는 움직임을 보완하기 위하여 등선량 곡선을 70%정도로 처방할 필요가 있다. 이때의 차이도 약 5 mm 미만이다. 이는 사이버나이프를 이용한 방사선수술 시 움직임 그 차체 보다 여유폭을 적게 줄 수 있다는 의미이며 이는 일반 방사선치료와 다른 점이라 할 수 있다.

• Radiation Oncology Journal
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• 제10권1호
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• pp.85-93
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• 1992

수술중 방사선치료를 환자에 적용하기에 앞서 본원이 보유하고있는 LID를 이용한 전자선의 선량분포 특성을 연구하였다. 이러한 선량 특성에 대한 자료는 적절한 Cone의 모양이나 크기, 에너지를 결정하게하며 빠르고 정확한 계산을 위하여 필요하다. 따라서, 본 저자들은 3-Dimensional Water Phantom Dosimetry System를 이용하여 Cone의 크기, Cone의 모양, 보상필터 사용 유무에 따라 Cone의 출력인자, 조직표면선량, 선축상 최대치 지점, $90\%$의 깊이, 대칭도와 편평도, SSD 보상인자, 선량분포 등을 측정하여 다음과 같은 결과를 얻었다. 1) Cone의 출력인자는 Cone모양에 따라 각각 측정하였으며 Cone의 크기와 에너지가 작을수록 급격하게 감소하는 결과를 보였다. 2) 보상 필터의 하나인 Flattening Filter를 사용한 결과 포면 선량이 6 MeV, 9 MeV, 12 MeV에 대하여 각각 $85.3\%$, $89.2\%$, $93.4\%$였고, 이 보상 필터를 사용하므로 선량률과 beam의 투과율은 감소하지만 치료부위에 따라 beam의 모양을 변형시키며 특히, 표면선량을 $90\%$나 그 이상으로 증가시킬수 있었다. 3) 3차에 걸친 beam의 collimation과 보상 필터를 결합하여 사용한 결과 매우 좋은 beam의 균일성과 편평도 뿐만아니라 $90\%$ 등선량곡선 넓이가 커지는 결과를 보였다. 4) 치료를 위하여 중요한 간격인 SSD 100cm에서 SSD 110cm까지의 출력인자는 측정치와 계산치가 Cone의 크기와 모양, 에너지에 따라 $1\~3\%$의 차이를 보였다.