研究者業績
基本情報
- 所属
- 藤田医科大学 医療科学部 講師
- 学位
- 博士(医療技術学)(名古屋大学)
- 研究者番号
- 00810748
- J-GLOBAL ID
- 201801015381626216
- researchmap会員ID
- B000307483
研究キーワード
4経歴
4-
2023年4月 - 現在
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2019年4月 - 2023年3月
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2018年4月 - 2019年3月
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2013年4月 - 2019年3月
学歴
3-
2015年4月 - 2018年3月
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2011年4月 - 2013年3月
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2007年4月 - 2011年3月
委員歴
1-
2021年4月 - 現在
受賞
7-
2024年9月
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2024年4月
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2022年11月
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2021年11月
論文
29-
Radiation Physics and Chemistry 229 112460-112460 2025年4月 査読有り
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Journal of Applied Clinical Medical Physics 2025年2月20日 査読有り筆頭著者責任著者Abstract Purpose The energy threshold is an important parameter for precise material identification employing photon‐counting techniques. However, in such applications, the appropriate energy threshold has not been clarified. Therefore, we aimed to determine the appropriate energy threshold range for precise material identification, focusing on effective atomic number (Z) values as an index. Methods The atomic number was estimated using a previously proposed algorithm and Monte Carlo simulations. This algorithm included three steps: calculating the attenuation factor from the incident photon counts on a photon‐counting detector, correcting the beam‐hardening effects, and estimating the atomic number from the attenuation factor index using the calibration curve. Monte Carlo simulations were performed to add Poisson noise to an ideal x‐ray spectrum. The total number of incident x‐rays was set in the range of 103–106. The x‐ray spectra were generated at tube voltages of 50–120 kV. Polymethyl methacrylate (Z = 6.5) and aluminum (Z = 13) were used for the analysis. The energy threshold was varied at intervals of 1 keV to estimate the atomic number. We evaluated the appropriate energy threshold range for accurately estimating the atomic number using the obtained atomic number data and statistical uncertainty under various conditions. Results The appropriate energy threshold range was found to be 31–38 keV for a tube voltage range of 50–120 kV. At this energy threshold, the atomic number can be estimated within an accuracy of ± 0.7 at 105 counts for the atomic number range of 6.5 (PMMA) to 13 (Al). Conclusions We found the appropriate energy threshold range. The findings of this study are expected to be useful for appropriately setting the energy threshold during precise material identification using photon‐counting detectors for clinical applications.
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Radiation protection dosimetry 2024年3月14日 査読有りThis study aimed to assess fetal radiation exposure in pregnant women undergoing computed tomography (CT) and rotational angiography (RA) examinations for the diagnosis of pelvic trauma. In addition, this study aimed to compare the dose distributions between the two examinations. Surface and average fetal doses were estimated during CT and RA examinations using a pregnant phantom model and real-time dosemeters. The pregnant model phantom was constructed using an anthropomorphic phantom, and a custom-made abdominal phantom was used to simulate pregnancy. The total average fetal dose received by pregnant women from both CT scans (plain, arterial and equilibrium phases) and a single RA examination was ~60 mGy. Because unnecessary repetition of radiographic examinations, such as CT or conventional 2D angiography can increase the radiation risk, the irradiation range should be limited, if necessary, to reduce overall radiation exposure.
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Physica Medica 118 2024年2月 査読有り筆頭著者責任著者
MISC
11-
Proceedings of the Twenty-Second EGS User's Meeting in Japan 19-24 2015年There has been a growing concern regarding exposure to superficial radiosensitive organs with the rapid increase of computed tomography examinations. Manufacturers have been developing various dose reduction methods in order to prevent harm to these organs. Our previous study revealed a unique phenomenon in X-ray computed tomography scanning, in which the maximum absorbed dose position shifts to a deeper region from the surface in a water cylindrical phantom. We considered that this result could be applied as a dose reduction method. Therefore, in this study, we investigate the tube voltage dependence of this unique phenomenon. The results show that the peak dose position shifts to a deeper region with increasing tube voltage. The superficial radiosensitive organs can thus be protected from peak dose exposure by adjusting the tube voltage.
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Proceedings of the Twenty-Second EGS User's Meeting in Japan 14-17 2015年近年の X 線 CT 装置には、患者の被ばく低減と画質の均一化を目的として、患者の体厚などに応じて管電流を変化させる管電流変調機構(Auto Exposure Control : AEC)が標準装備されている。そのため、モンテカルロシミュレーションを用いて患 者の被ばく線量について検討を行う場合、AEC の影響を考慮しなければならない。<br /> 本研究室ではこれまで、球形半導体検出器を用いて測定した管電流変調データを、 EGS5 に組み込んで人体ファントムの被ばく線量の取得を試みていたが、主に体表部 に近い位置に設置された検出器で、実測と計算の値が大きく異なる場合があった。<br /> そこで今回は、管球回転開始位置の違いによるスキャン中の回転軌道の違いが影響 しているのではないかと考え、回転開始位置の異なる実測変調データ数種を EGS5 に 組み込み、検証を行った。
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Radiological Physics and Technology 7(1) 133-140 2014年 査読有りThe longitudinal dose profile in a computed tomography dose index (CTDI) phantom had been studied by many researchers. The cross-sectional dose profile in the CTDI phantom, however, has not been studied. It is also important to understand the cross-sectional dose profile in the CTDI phantom for dose estimation in X-ray CT. In this study, the cross-sectional dose profile in the CTDI phantom was calculated by use of a Monte Carlo (MC) simulation method. A helical or a 320-detector-row cone-beam X-ray CT scanner was simulated. The cross-sectional dose profile in the CTDI phantom from surface to surface through the center point was calculated by MC simulation. The shape of the calculation region was a cylinder of 1-mm-diameter. The length of the cylinder was 23, 100, or 300 mm to represent various CT ionization chamber lengths. Detailed analyses of the energy depositions demonstrated that the cross-sectional dose profile was different in measurement methods and phantom sizes. In this study, we also focused on the validation of the weighting factor used in weighted CTDI (CTDIw). As it stands now, the weighting factor used in CTDI w is (1/3, 2/3) for the (central, peripheral) axes. Our results showed that an equal weighting factor, which is (1/2, 1/2) for the (central, peripheral) axes, is more suitable to estimate the average cross-sectional dose when X-ray CT dose estimation is performed. © Japanese Society of Radiological Technology and Japan Society of Medical Physics 2013.
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放射線防護分科会会誌 (35) 48-48 2012年10月4日
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Proceedings of the Nineteenth EGS Users' Meeting in Japan 48-52 2012年10月In this study, the absorbed dose for organs in infant, child, and adult patients undergoing head computed tomography (CT) scans was determined. The CT examinations were simulated using the Electron Gamma Shower ver. 5 (EGS5) Monte Carlo code. The eye lens dose among child and infant patients was higher than that among adult patients by 15.0% and 69.7%, respectively. The effectiveness of a bismuth shield in reducing the eye lens dose for children undergoing head X-ray head CT scans was also evaluated. Application of a bismuth shield over the eyes of children undergoing head X-ray CT reduced the eye lens dose by 47.6% from the dose value in the case wherein shielding was not used. The use of metallic shields was found effective in reducing the radiation dose to children.
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Proceedings of the Nineteenth EGS Users' Meeting in Japan 1-3 2012年10月In this study, we validated the effectiveness of using a message passing interface (MPI) method in reducing computation time and enhancing calculation accuracy. A chest and abdominal X-ray computed tomography scan was simulated. Our results indicated that the MPI method was accurately incorporated into the Electron Gamma Shower ver. 5 (EGS5) MC code. The MPI method could reduce computation time from 34 hours to 6 hours. We believe that MC simulation is going to be used widely. Therefore, incorporating the MPI method into EGS5 is very useful for EGS5 users.
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Proceedings of the Eighteenth EGS User's Meeting in Japan 58-61 2011年10月
講演・口頭発表等
47担当経験のある科目(授業)
11-
2023年4月 - 現在医療安全管理学 (藤田医科大学)
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2023年4月 - 現在放射線計測学Ⅱ (藤田医科大学)
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2023年4月 - 現在モンテカルロシミュレーション (藤田医科大学)
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2022年4月 - 現在放射線医学概論(一般撮影、血管造影検査) (藤田医科大学)
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2020年4月 - 現在診療画像技術学Ⅱ(血管造影検査) (藤田医科大学)
所属学協会
2共同研究・競争的資金等の研究課題
6-
日本学術振興会 科学研究費助成事業 2024年4月 - 2027年3月
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日本学術振興会 科学研究費助成事業 2023年4月 - 2026年3月
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日本学術振興会 科学研究費助成事業 2022年4月 - 2025年3月
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日本学術振興会 科学研究費助成事業 2019年4月 - 2022年3月
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藤田医科大学 教員研究助成費(若手) 2020年4月 - 2021年3月