• 대한방사선기술학회지:방사선기술과학
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• 제45권4호
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• pp.299-304
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• 2022

This study uses the 'S-align' function to present a reference value of the X-ray tube angle for the realization of an image similar to that of the chest PA image during chest AP radiography. This study targeted dummy phantom and used a 17"×17" DR image receptor. The irradiation conditions were 110 kVp, 160 mA, 50 ms, and the distance between the central X-ray and the image receptor was set to 180 cm and 110 cm, respectively. The end of the catheter was placed at the 11th thoracic height to indicate the nasogastric tube. In the case of lung apex length measurement, the mean value of measurement was 30.53±0.47 in PA. T 0°, TCA 5~25°, TCE 5~15° were 21.07±0.29, 27.60±0.21, 34.13±0.44, 39.86±0.31, 45.96±0.61 mm, 54.13±0.37 mm, 16.16±0.46 mm, 9.81±0.35 mm, 2.75±0.30 mm, respectively. For the depth of the catheter end, the average value measured at PA was 6.70±0.31 mm. T 0°, TCA 5~25°, TCE 5~15° were 15.72±0.38 mm, 24.10±0.50 mm, 29.24±0.86 mm, 34.35±0.35 mm, 41.06±1.08 mm, 48.07±0.38 mm, 12.85±0.25 mm, 7.92±0.36 mm, 3.01±0.39 mm, respectively. The length of the lung apex was similar to that of chest PA when the angle of incidence was adjusted from 5° to 10° in the leg direction, and the depth of the catheter tip was most similar when the X-ray tube angle was incident at 10° in the head direction. Therefore, To change the X-ray tube angle according to the purpose of the examination during the chest AP radiography using 'S-align' function is considered necessary.

• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2003년도 제27회 추계학술대회
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• pp.69-69
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• 2003

Flat panel based digital radiography (DR) systems have recently become useful and important in the field of diagnostic radiology. For DRs with amorphous silicon photosensors, CsI(TI) is normally used as the scintillator, which produces visible light corresponding to the absorbed energy. The visible light photons are converted into an electric signal in the amorphous silicon photodiode. In order to produce good quality images, we need to understand the detailed behavior of DR detectors in radiation. We, therefore, investigated the relationship between DR outputs and X -ray in terms of absorbed energy, using the SPEC-78, X-ray energy spectrum model. We calculated the total filtration of X-ray equipment measuring air exposure and this value was used in the calculation of absorbed energy. The relationship between DR output and the absorbed energy of the X-ray was obtained by matching the absorbed energy with pixel values of real images under various conditions. It was found that the relationship between these two values was almost linear. The results were verified using phantoms made of water and aluminium. The pixel value of the phantom image was estimated and compared with previous results under various conditions. The estimated pixel value coincided with the results, although the effect of scattered photons introduced some errors.

• 대한방사선기술학회지:방사선기술과학
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• 제40권1호
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• pp.71-78
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• 2017

디지털 방사선영상 시스템에서 산란선은 피검사체와 엑스선의 반응에 의해 발생하는 근원적인 현상이다. 방사선 투사영상은 일차선에 의해 형성되는 감쇠정보를 영상화 하므로 산란선은 투사영상에서 노이즈로써 작용한다. 본 연구에서는 다양한 검사조건에서 발생하는 산란선을 빔 저지체(beam stopper)를 이용하여 정량화하고 동시에 반 산란 격자의 효과를 확인하였다. 또한 산란선이 영상의 품질에 미치는 영향을 확인하기 위해 산란선에 의해 저하되는 대조도 대 잡음비를 측정하였다. 본 연구를 통해 산란선은 피검사체의 두께 및 공기층(air gap)에 지배적인 경향을 가짐을 확인하였다. 또한 산란선은 영상의 대조도를 현격히 저하시킴을 정량적으로 측정하였다. 산란선을 저감하기 위해 격자를 장착함으로써 상당량의 산란선을 저감할 수 있었으나 여전히 두꺼운 피검사체에 대해 많은 양의 산란선이 남아 있음을 확인하였다. 본 연구에서는 산란선을 정량화 하는 방법론을 제시하였으며, 향후 시스템의 최적화에 중요한 역할을 할 수 있을 것으로 기대된다.

• Imaging Science in Dentistry
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• 제38권1호
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• pp.49-56
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• 2008

Purpose: Diagnostic estimation of destruction and formation of bone has the typical limit according to capacity of x-ray generator and image detector. So the aim of this study was to find out how much it can reproduce the shape and the density of bone in the case of using recently developed dental type of cone beam computed tomography, and which image is applied by new detector and mathematic calculation. Materials and Methods: Cone beam computed tomography (PSR 9000N, Asahi Roentgen Ind. Co., Ltd., Japan) and soft x-ray radiography were executed on dry mandible that was already decalcified during 5 hours, 10 hours, 15 hours, 20 hours, and 25 hours. Estimating and comparing of those came to the following results. Results: The change of inferior border of mandible and anterior border of ramus in the region of cortical bone was observed between first 5 and 10 hours of decalcification. The reproduction of shape and density in the region of cortical bone and cancellous bone can be hardly observed at cone beam computed tomography compared with soft x-ray radiography. The difference of decrease of bone density according to hours of decalcification increase wasn't reproduced at cone beam computed tomography compared with soft x-ray radiography. Conclusion: CBCT images revealed higher spatial resolution. However, contrast resolution in region of low contrast sensitivity is the inferiority of images' property.

• Nuclear Engineering and Technology
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• 제55권2호
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• pp.655-668
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• 2023

In radiography, an antiscatter grid is a well-known device for eliminating unexpected x-ray scatter. We investigate a new stationary grid artifact suppression method based on a nonsubsampled contourlet transform (NSCT) incorporated with Gaussian band-pass filtering. The proposed method has an advantage that extracts the Moiré components while minimizing the loss of image information and apply the prior information of Moiré component positions in multi-decomposition sub-band images. We implemented the proposed algorithm and performed a simulation and an experiment to demonstrate its viability. We did this experiment using an x-ray tube (M-113T, Varian, focal spot size: 0.1 mm), a flat-panel detector (ROSE-M Sensor, Aspenstate, pixel dimension: 3032 × 3800 pixels, pixel size: 0.076 mm), and carbon graphite-interspaced grids (JPI Healthcare, 18 cm × 24 cm, line density: 103 LP/inch and 150 LP/inch, ratio: 5:1, focal distance: 65 cm). Our results indicate that the proposed method successfully suppressed grid artifacts by reducing them without either reducing the spatial resolution or causing negative side effects. Consequently, we anticipate that the proposed method can improve image acquisition in a stationary grid x-ray system as well as in extended x-ray imaging.

• 대한방사선기술학회지:방사선기술과학
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• 제35권4호
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• pp.309-314
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• 2012

Digital Radiography(DR) 시스템은 임상현장에서 아날로그 시스템을 대체하고 널리 이용되고 있다. DR을 이용하여 얻어진 X선 영상의 해상력을 결정짓는 요소에는 이용되는 검출기의 고유 해상력, 피사체의 대조도 및 특성, X선 선질, X선원의 산란, DR 검출기의 성능, X선 변환효율 및 초점의 크기, 피사체의 움직임 등이 있다. DR 검출기를 구성하는 요소에는 X선 포획 요소, 커플링 요소, 정보수집 요소가 있는데 이들은 시스템의 성능에 영향을 미치며, 그 성능은 해상력으로 평가된다. 의료영상 시스템의 해상력은 촬영대상물의 조직 간의 해부학적 영상을 구분하는 능력을 나타낸다. 해상력 평가를 위해 Modulation Transfer Function(MTF)이 보편적으로 이용되고, MTF는 입력 공간주파수 성분에 대한 출력 공간주파수 성분의 비를 나타내는데, 수학적으로 MTF는 Point Spread Function(PSF) 입력에 대한 시스템의 주파수 응답이며 Edge Phantom을 이용한 결과 영상에서 추출된 Line Spread Function(LSF)을 Fourier Transform하면 얻을 수 있다. 일반적으로 임상현장에서 의료영상시스템의 이용 및 관리의 책임은 방사선사가 맡고 있지만, MTF를 측정하기 위해서는 공학적, 수학적 기초 및 C, Fortran, Matlab등의 프로그램 작성 능력이 필요하기 때문에 비 공학도는 정확한 측정이 불가능하다. 의료영상 시스템의 성능 관리 및 최상의 상태를 유지하기 위해 시스템의 성능평가가 이뤄져야 하는데, 이를 위해 본 연구에서는 비공학도가 해상력 성능평가를 할수 있도록 ImageJ 및 Excel을 이용하여 해상력 평가를 할 수 있도록 방법을 제시하고, 제안된 방법을 이용해 계산된 결과와 프로그래밍을 이용해 계산된 결과의 비교를 통해 본 논문에서 제시하는 방법의 유용성을 확인하였다.

• 대한방사선기술학회지:방사선기술과학
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• 제39권4호
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• pp.501-507
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• 2016

본 연구는 손, 머리, 허리측방향 등에 대한 X선 촬영조건(kVp, mAs)으로 SID 50cm, 1m, 2m에서 발생되는 1차 X선이 보호앞치마를 어느 정도 투과하는지를 알아보았고, 그 결과는 다음과 같다. 첫째, 손 X선 촬영조건의 1차X선은 0.3mmPb 보호앞치마로 차폐할 경우 선량을 약 270배 줄일 수 있으나 SID 50cm, 1m, 2m에서 보호앞치마를 각각 0.120, 0.043, 0.012mR 수준으로 투과한다. 둘째, 머리 X선 촬영조건의 1차X선은 0.3mmPb 보호앞치마로 차폐할 경우 선량을 약 22배 줄일 수 있으나 SID 50cm, 1m, 2m에서 보호앞치마를 각각 13.191, 4.821, 1.388mR 수준으로 투과한다. 셋째, 허리측방향 X선 촬영조건의 1차X선은 0.3mmPb 보호앞치마로 차폐할 경우 선량을 약 13배 줄일 수 있으나 SID 50cm, 1m, 2m에서 보호앞치마를 각각 77.844, 27.406, 8.606mR 수준으로 투과한다. 따라서 X선 검사 시 촬영실 내에 있는 관계자들은 1차X선이 도달하는 모든 공간에서 보호앞치마만을 착용한 채 머물러 있어서는 안 되며, 부득이하게 촬영실 안에 머물러 있어야 할 경우 보호앞치마 착용과 함께 두꺼운 납이 내장된 차폐칸막이 뒤에 안전하게 피해야 한다.

• 정보처리학회논문지B
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• 제11B권3호
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• pp.275-280
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• 2004

본 논문은 디지털 방사선 영상에 영상처리기법을 이용하여 기존의 수동적인 방법으로 개인차를 유발했던 차영상 진단방법을 자동화하는 알고리즘 방법을 제안한다. 이를 위해 차영상 획득 이전에 수행될 투 영상의 정렬방법과 치과용 디지털 방사선영상내의 구조적 특징을 이용하여 관심영역을 선정할 수 있는 방법론을 제안하고, 이를 이용하여 영역에 대한 차정보 표시 및 이에 대한 수치적 근거를 제시함으로써 기존의 방법이 갖지 못한 결과의 일관성 및 객관성을 갖도록 하였다. 구현결과 인간의 시각으로 판별하기 어려운 미세한 차이의 표시 및 환부의 이상발생여부를 확연히 구분할 수 있었다.

• 대한디지털의료영상학회논문지
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• 제15권2호
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• pp.31-37
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• 2013

Incident X-ray angles of weight bearing foot AP radiography which differ in each medical institution were compared. Optimal angles were derived from the study and suggested as basic data for clinical application. 19 patients with no abnormality on right foot took part in the study from June 2013 to July 2013. Weight bearing foot AP radiography in the correct position was examined with the incident X-ray angles of $10^{\circ}$, $15^{\circ}$, $20^{\circ}$, $25^{\circ}$, $30^{\circ}$, and $35^{\circ}$. All the images were evaluated subjectively by 5 radiological technologists of over 15 year work experience using Likert scale as 1 for 'very poor', 2 for 'poor', 3 for 'fair', 4 for 'good', 5 for 'very good', 6 for 'excellent', and analyzed with ANOVA and Scheffe. Image quality was the most optimal at $20^{\circ}$ as 4.53, and relatively good at $25^{\circ}$ as 4.38 and at $30^{\circ}$ as 4.18. $35^{\circ}$ and $10^{\circ}$ were relatively poor. The average points of 6 groups indicated statistically significant difference (p<.01). In the post-mortem, 3 subgroups showed no statistically significant difference, and the average point of the groups of $20^{\circ}$, $25^{\circ}$, $30^{\circ}$was evaluated relatively higher than the other 2 groups. An optimal incident X-ray angle within the range from $20^{\circ}$ to $30^{\circ}$ for weight bearing foot AP radiography could make it possible to obtain the image of high diagnostic value and would be useful for clinical application in the future.

• 대한방사선기술학회지:방사선기술과학
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• 제23권1호
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• pp.13-19
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• 2000

We have presented with the "A study on overexposure rate according to over-density in chest X-ray radiography(I)" last year. In this report, We could calculate the entrance skin dose from chest X-ray film density the formula $I_0=Ix/e^{-{\mu}x}{\times}mG$, (mG is Bucky factor) was used to deliver the skin dose. At that time, There was two problems that the Bucky factor from maker was not equal to field experience and the field size influenced on the Attenuation Rate. The experiment of Bucky factor was done from film method and retried the Attenuation Rate of Acryle phantom according to Good & Poor geometry. As the results, The Bucky factor from maker higher than in this experiments $30{\sim}40%$. The Attenuation Rate in good geometric condition brings about a little alteration compare with poor geometric condition. In the field experiment, we could get the chest image with very low entrance skin radiation dose $29.3{\mu}Sv$, especially with air gap methode, the entrance skin dose was detected $10{\mu}Sv$.