• 한국콘텐츠학회논문지
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• 제12권7호
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• pp.255-260
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• 2012

흉부 X-선 촬영 시 피사체의 유무, 촬영실내 X선관과 수광계 (image receptor), 환자 보기창 앞, 환자대기실 출입문 외측, 출입문 개폐여부, 방사선 관계 종사자 출입문 외측, 방사선 관계 종사자 출입문 개폐여부 등으로 구분하여 공간산란선발생을 알아보기 위한 연구로 공간산란선발생에 대한 연구 결과 피사체가 있을 때 수광계 (image receptor) 위치; Chest PA: $663{\pm}3.4$ mR/h, Chest Lateral: $2,067{\pm}3.7$ mR/h, X선관 위치; Chest PA: $293{\pm}2.1$ mR/h, Chest Lateral: $927{\pm}1.9$ mR/h, 환자대기실 출입문 외측 열고; Chest PA: $17{\pm}1.6$ mR/h, Chest Lateral: $88{\pm}2.6$ mR/h, 방사선 관계 종사자 촐입문 외측 열고; Chest PA: $3{\pm}1.6$ mR/h, Chest Lateral: $19{\pm}1.6$ mR/h), 피사체의 두께가 두꺼울수록 각 각의 측정지점에서 산란선 발생이 많았고, 출입문을 닫고 측정한 경우 산란선이 더 적었다. 그러므로 방사선 관계종사자는 촬영실내 산란선 분포에 대한 정확한 정보를 인지하여 불필요한 방사선 피폭을 줄일 수 있도록 노력해야 한다.

• 전자통신동향분석
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• 제34권5호
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• pp.1-13
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• 2019

In modern times, X-ray imaging has become a necessary tool for early diagnosis, quality control, nondestructive testing, and security screening. X-ray imaging equipment generally comprises an X-ray generator and an image sensor. Most commercially available X-ray generators employ filament-thermionic electron-based X-ray tubes, thus demonstrating typical analog behavior, such as slow response and large stray X-rays. Furthermore, digital X-ray sources, which have been studied extensively using field electron emitters manufactured from nanometer-scale materials, provide fast and accurately controlled ultra-shot X-rays. This could usher in a new era of X-ray imaging in medical diagnosis and nondestructive inspections. Specifically, digital X-ray sources, with reduced X-ray dose, can significantly improve the temporal and spatial resolution of fluoroscopy and computed tomography. Recently, digital X-ray tube technologies based on carbon nanotubes, developed by Electronics and Telecommunications Research Institute, have been transferred to several companies and commercialized for dental imaging for the first time.

• 천문학논총
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• 제15권spc1호
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• pp.113-118
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• 2000

A magnetic cataclysmic variable has a rotating magnetic white dwarf which accretes matter from its late type companion. Kim & Beuermann (1995) presented a phenomenological model of the accretion from its surrounding structure e.g., a disk into the magnetosphere of the white dwarf, and presented results for the spin modulated X-ray spectrum and light curves. Using this model, we calculate the optical continuum and line emission which result from reprocessing of X-rays in the accretion stream within the magnetosphere. Penning (1985) suggested the observed spin-modulated radial-velocity variations might result from reprocession of X-rays in the disk. We, however, find the radiation can be originated from the magnetosphere accretion stream. We use the same geometrical model to calculate the optical and the X-ray behaviour. The results from the two wavelength bands are internally consistent. We conclude that this approach will increase the diagnostic accuracies of the results.

• 한국인쇄학회지
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• 제20권2호
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• pp.153-160
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• 2002

Two different commercial brand X-ray films are used for examining possible differences caused by different target distances when the patients are examined with highenergy X-rays. 6MV- and 15MV X-rays are tested at four different target distances. The films on which the radiation amounts are gradually increased using H$_2$O phantoms are developed by an automatic developing machine to be analysed in the image densities. Characteristic curves have similar shapes for different conditions but for the 130cm target distance. ${\gamma}$ values and average image densities per the illuminated radiation are used to analyse the differences.

• 방사선산업학회지
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• 제11권3호
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• pp.167-171
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• 2017

This study examined the effectiveness degree of a protective apron that is taken not to be exposed to the first ray or scattered rays, for X-ray of thick subject like lateral lumbar, and the results are as follows; First, spatial dose by scattered rays is shielded by 3 mmPb protective apron, 86.8% at a distance of 50 cm, 92.7% at 100 cm, and 95.6% at 200 cm, when minimizing the field size, while 89% at a distance of 50 cm, 92.3% at 100 cm, and 95.2% at 200 cm, when maximizing the field size. Second, 1st exposure dose is shielded by 3 mmPb protective apron, 93.7% at a distance of 50 cm, 94.4% at 100 cm, and 93.6% at 200 cm, when minimizing the field size, while 93.7% at a distance of 50 cm, 93.6% at 100 cm, and 94.2% at 200 cm, when maximizing the field size.

• 대한방사선기술학회지:방사선기술과학
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• 제16권1호
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• pp.107-115
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• 1993

In this study, to develop highly sensitive radiation sensors, $CaSO_4$ : Tm phosphors and its disc-type TLD elements embedded PTFE(polytetrafluoroethylene) are fabricated. The highest sensitivity of $CaSO_4$ : Tm phosphors is obtained when phosphors have been doped with 0.5mol % Tm and sintered in atmosphere at $600^{\circ}C$ for two hours. Fabricated disc-type elements are made from a homogeneous mixture of phosphors and PTFE powder. They are first cold-pressed and then polymerized at $370^{\circ}C$ in air for one hour. The dose dependence of the prepared $CaSO_4$ : Tm TLD radiation sensors is linear within the range of $100{\mu}Gy{\sim}10Gy$ for X-rays and ${\gamma}-rays$. The response of $CaSO_4$ : Tm to 30keV X-rays is ten times higher than that of 1.25MeV $^{60}Co\;{\gamma}-rays$. The fading rate of the main peak is about 2% per a month. The spectral peaks of TL emission spectrum are at about 350nm and 475nm. The $CaSO_4$ : Tm TLD radiation sensors prepared in this work may be used as radiation dosimeter for personal and environmental monitoring because of their high sensitivity and little fading.

• Nuclear Engineering and Technology
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• 제50권6호
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• pp.923-928
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• 2018

We developed a compact gamma camera based on a modified uniformly redundant array coded aperture to investigate the position of a $UO_2$ pellet emitting characteristic X-rays (98.4 keV) and ${\gamma}-rays$ (185.7 keV). Experiments using an only-mask method and an antimask subtractive method were conducted, and the maximum-likelihood expectation maximization algorithm was used for image reconstruction. The images obtained via the antimask subtractive method were compared with those obtained using the only-mask method with regard to the signal-to-noise ratio. The reconstructed images of the antimask subtractive method were superior. The reconstructed images of the characteristic X-rays and the ${\gamma}-rays$ were combined with the obtained image using the optical camera. The combined images showed the precise position of the $UO_2$ pellet. According to the self-absorption ratios of the nuclear material and the minimum number of effective events for image reconstruction, we estimated the minimum detection time depending on the amount of nuclear material.

• Radiation Oncology Journal
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• 제21권4호
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• pp.322-329
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• 2003

목적 .: 고에너지 X-선의 표면 선량과 선량보강(build-up) 영역에서의 선량 분포는 일반적으로 방사선 계측에 사용되는 전리함 측정기로는 정확한 선량 분포를 얻기가 매우 어렵다. 본 연구는 고에너지 X-선 선량 계측에 보편적으로 사용되고 있는 여러 측정기를 이용하여 팬톰 표면에서의 흡수선량과 최대 선량 지점(d$_{max}$)을 측정하여 측정기 사이의 정확성을 비교 분석하고, 각 치료 기관에서 보편적으로 사용되는 측정기 중 표면 선량 측정에 적절한 측정장치를 제안하고 그 유용성을 제시하고자 한다. 대상 및 방법 : 본 실험에서는 6 MV와 IS MV X-선에 대해 조사면이 10$\times$10 cm$^{2}$, SSD=100 cm에서 TLD, 팀블형전리함(thimble type ion chamber), 다이오드 검출기, 다이아몬드 검출기와 Markus 평행판 전리함 등을 이용하여 심부선량백분율(percent depth dose: PDD)을 측정하여, 표면 선량(suface dose)과 최대 선량 지점(dnu)을 비교 분석하고, 또한 TLD 측정 시와 동일 조건으로 Monte Cario 계산을 실행하여 TLD의 측정 결과와 비교하였다. 결과: 6 WV와 IS MV X-선에 대해 Markus 평행판 전리함을 이용하여 측정한 표면 선량은 각각 29.31$\%$와 23.36$\%$으로 측정되었으며, TLD는 37.17$\%$와 24.06$\%$, 다이아몬드 검출기는 34.78$\%$와 24.06$\%$, 다이오드 검출기는 38.18$\%$와 27.8$\%$, 팀블형 전리함은 47.92$\%$와 36.06$\%$ 였으며, Monte Cario 계산에 의한 표면 선량 값은 S MV X-선에 대해 TLD 측정 시와 동일한 조건으로 팬톰 내에 가상적인 TLD를 삽입한 경우 36.22$\%$로 실제 측정값 37.17$\%$와 유사하였다. 최대 선량 지점의 깊이는 모든 측정기에서 6 MV X-선에 대하여 14$\~$16 mm, IS MV X-선에서는 27$\~$29 mm사이의 측정기에 따라 작은 차이를 보였다. 결론 : 표면 선량의 경우에는 측정기에 따라 현저한 차이를 보였으며 Markus 평행판 전리함이 사용된 측정기 중가장 정확한 결과를 보였고, 팀블형 전리함의 경우 다른 측정기에 비해 약 10$\%$ 이상 높은 선량을 보여 피부 표면에 가까이 위치한 종양에 대한 방사선 치료 계뵉 시에는 임상에서 가장 보편적으로 사용되고 있는 팀블형 전리함의 선량 값을 그대로 사용하기에는 많은 오류가 발생하므로 가능한 표면 선량 측정에 적절한 측정기를 선택하여 사용하거나 측정기 특성을 고려한 보정이 필요할 것으로 생각된다. 최대 선량 지점(d$_{max}$)의 결과는 모든 측정기에서 비슷한 결과를 나타내고 있어 본 실험에서 사용한 모든 측정기는 그 특성에 상관없이 최대 선량 지점 측정에 사용이 가능함을 알 수 있었다.

• 대한의용생체공학회:의공학회지
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• 제10권3호
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• pp.331-342
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• 1989

This paper presents a new algorithm that extracts lung region in X-Rays and enhance.j the region. Comparing to prior algorithms that enhance whole X-Ray image, this algorithm leads more effective results. For this algorithm extracts lung region first, and enhances the lung region excluding parameters of other region. For choosing optimal threshold, we compare OTSU's mothod with the proposed method. We obtain lung boundary using contour following algorithm and Rray level searching method in gray level rescaled image. We Process histogram equalization in lung region and obtain enhanced lung image. By using the proposed algorithm, we obtain lung region effectively in chest X-Ray that need in medical image diagnostic system.

• Journal of the Korean Physical Society
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• 제73권12호
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• pp.1895-1898
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• 2018

The mechanical properties of Al, Ti, Fe, and Cu metals p-type Si, and n-type Si were investigated by using coincidence Doppler broadening (CDB) positron annihilation spectroscopy. The samples in this experiment were irradiated by using X-rays at generating powers for up to 9 kW. The data taken after the irradiation showed all the characteristic features predicted from defects with vacancies. The S parameter values of the metals were generally less than those of semiconductors such as p-type Si and n-type Si. The relationship between n-type Si and p-type Si were more affected when n-type Si rather than p-type Si was irradiated with X-rays.