Curriculum Vitaes
Profile Information
- Affiliation
- Professor, School of Health Sciences Clinical Collaboration Unit Department of Medical Equipment Engineerinig, Fujita Health University
- Degree
- Ph.D.(Mar, 1998, Fujita Health University)
- J-GLOBAL ID
- 200901009745424797
- researchmap Member ID
- 1000254980
Research Areas
1Committee Memberships
3-
Apr, 2003 - Jun, 2019
-
Apr, 2013 - Apr, 2016
-
Apr, 2009 - Apr, 2013
Awards
3Papers
138-
Radiation protection dosimetry, Mar 14, 2024 Peer-reviewedThis 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.
-
Physica medica : PM : an international journal devoted to the applications of physics to medicine and biology : official journal of the Italian Association of Biomedical Physics (AIFB), 118 103215-103215, Jan 14, 2024 Peer-reviewedPURPOSE: Organ dose evaluation is important for optimizing cone beam computed tomography (CBCT) scan protocols. However, an evaluation method for various CBCT scanners is yet to be established. In this study, we developed scanner-independent conversion coefficients to estimate organ doses using appropriate peak dose (f(0)) indices. METHODS: This study included various scanners (angiography scanners and linear accelerators) and protocols for the head and body (thorax, abdomen, and pelvis) scan regions. f(0) was measured at five conventional positions (center position (f(0)c) and four peripheral positions (f(0)p) at 90° intervals) in the CT dose index (CTDI) phantom. To identify appropriate measurement positions for organ dose estimation, various f(0) indices were considered. Organ doses were measured by using optically stimulated luminescence dosimeters positioned in an anthropomorphic phantom. Thereafter, the conversion coefficients were calculated from each obtained f(0) value and organ or tissue dose using a linear fit for all scanners, and the coefficient of variation (CV) of the conversion coefficients was calculated for each organ or tissue. The f(0) index with the minimum CV value was proposed as the appropriate index. RESULTS: The appropriate f(0) index was determined as f(0)c for the body region and a maximum of four f(0)p values for the head region. Using the proposed conversion coefficients based on the appropriate f(0) index, the organ/tissue doses were well estimated with a mean error of 14.2% across all scanners and scan regions. CONCLUSIONS: The proposed scanner-independent coefficients are useful for organ dose evaluation using CBCT scanners.
-
Biomedical physics & engineering express, 10(1), Dec 29, 2023 Peer-reviewedEffective dose is sometimes used to compare medical radiation exposure to patients and natural radiation for providing explanations about radiation exposure to patients, but its calculation is lengthy and requires dedicated measuring devices. The purpose of this study was to identify the most suitable conversion coefficient for conversion of easily measurable dose to effective dose in posterior-anterior chest radiography, and to evaluate its accuracy by direct measurement. We constructed an examination environment using Monte Carlo simulation, and evaluated the variation in conversion coefficients from incident air kerma (IAK), entrance-surface air kerma (ESAK), and air kerma-area product (KAP) to effective dose when the irradiation field size and radiation quality were changed. Effective doses were also measured directly using thermoluminescence dosimeters and compared with the effective dose obtained from conversion coefficients. The KAP conversion coefficient most effectively suppressed the effect of irradiation field size, and was then used to set conversion coefficients for various half-value layers. The optimal conversion coefficient was 0.00023 [mSv/(mGy·cm2)] at 120 kVp (half-value layer = 5.5 mmAl). Evaluation of the direct measurements obtained with various radiation qualities revealed that the accuracy of the conversion coefficient was maintained at ≤ 11%. The proposed conversion coefficient can be easily calculated even in facilities that do not have equipment for measuring effective dose, and might enable the use of effective dose for providing explanations about radiation exposure to patients.
-
Physical and engineering sciences in medicine, 46(1) 141-150, Mar, 2023 Peer-reviewedWe aimed to verify whether the image quality of large low-contrast objects can be improved using visual model-based iterative reconstruction (VMR) while maintaining the visibility of conventional filtered back projection (FBP) and reducing radiation dose through physical and visual evaluation. A 64-row multi-slice CT system with SCENARIA View (FUJIFILM healthcare Corp. Tokyo, Japan) was used. The noise power spectrum (NPS), task-based transfer function (TTF), and signal-to-noise ratio (SNR) were physically evaluated. A low contrast object as a substitute for a liver mass was visually evaluated. In the noise measurement, STD1 showed an 18% lower noise compared to FBP. STR4 was able to reduce noise by 58% compared to FBP. The NPS of VMR was similar to those of FBP from low to high spatial frequency. The NPS of VMR reconstructions showed a similar variation with frequency as FBP reconstructions. STD1 showed the highest 10% TTF, and higher 10% TTF was observed with lower VMR level. The SNR of VMR was close to that of FBP, and higher SNR was observed with higher VMR level. In the results of the visual evaluation, there was no significant difference in visual evaluation between STD1 and FBP (p = 0.99) and between STD2 and FBP (p = 0.56). We found that the NPS of VMR images was similar to that of FBP images, and it can reduce noise and radiation dose by 25% and 50%, respectively, without decreasing the visual image quality compared to FBP.
-
Journal of Applied Clinical Medical Physics, Dec 22, 2022 Peer-reviewed
Misc.
133-
電気・電子・情報関係学会東海支部連合大会講演論文集(CD-ROM), 2015 ROMBUNNO.PO1-52, Sep 18, 2015
-
Journal of applied clinical medical physics, 15(5) 4823-4823, Sep 7, 2014 Peer-reviewedWe modified the Imaging Performance Assessment of CT scanners (ImPACT) to evaluate the organ doses and the effective dose based on the International Commission on Radiological Protection (ICRP) Publication 110 reference male/female phantom with the Aquilion ONE ViSION Edition scanner. To select the new CT scanner, the measurement results of the CTDI100,c and CTDI100,p for the 160 (head) and the 320 (body) mm polymethylmethacrylate phantoms, respectively, were entered on the Excel worksheet. To compute the organ doses and effective dose of the ICRP reference male/female phantom, the conversion factors obtained by comparison between the organ doses of different types of phantom were applied. The organ doses and the effective dose were almost identical for the ICRP reference male/female and modified ImPACT. The results of this study showed that, with the dose assessment of the ImPACT, the difference in sex influences only testes and ovaries. Because the MIRD-5 phantom represents a partially hermaphrodite adult, the phantom has the dimensions of the male reference man including testes, ovaries, and uterus but no female breasts, whereas the ICRP male/female phantom includes whole-body male and female anatomies based on high-resolution anatomical datasets. The conversion factors can be used to estimate the doses of a male and a female accurately, and efficient dose assessment can be performed with the modified ImPACT.
-
放射線防護分科会会誌, (36) 42-43, Apr 11, 2013
-
Nihon Hoshasen Gijutsu Gakkai zasshi, 69(1) 1-9, Jan, 2013 Peer-reviewed
-
放射線防護分科会会誌, (27) 67-67, Oct 23, 2008
-
日本放射線技術學會雜誌, 63(9) 997-997, Sep 20, 2007
-
日本放射線技術學會雜誌, 63(9) 997-997, Sep 20, 2007
-
日本放射線技術學會雜誌, 63(9) 1003-1003, Sep 20, 2007
-
日本放射線技術學會雜誌, 63(9) 999-999, Sep 20, 2007
-
日本放射線技術學會雜誌, 63(9) 1002-1003, Sep 20, 2007
-
日本放射線技術學會雜誌, 63(9) 1035-1035, Sep 20, 2007
-
医科器械学, 77(5) 293-301, May 1, 2007The development of multi-detector computed tomography (MDCT) scanners has contributed to the swift acquisition of highly detailed three-dimensional images that were formerly unobtainable from the single-detector CT (SDCT) devices. Obtaining more detailed image data inevitably causes an increase of X-ray dose, and that varies with, the scanning procedures and type of devices. We measured the X-ray doses from currently used CT devices (60 devices in 50 facilities) for scans of the head and abdomen. X-ray dose evaluation was performed by using the CTDIvol indicated in the IEC standards. An ionization-chamber CT dosimeter corrected to the national standard was used to the dosimetry of X-ray, and acrylic cylinders of diameter 16 cm for head scanning and 32 cm for abdominal scanning used as the phantoms. The results showed that the CTDIvol obtained by using air kerma in PMMA was an average of 62.48 mGy for head scans and 16.76 mGy for abdominal scanning. The difference of the CTDIvol between facilities was around to three standard deviation for both head and abdominal scanning. The X-ray dose was greatest for eight-row devices, and did not increase substantially even for 16-row and 64-row multi-detector devices. On the contrary, it showed a tendency to decrease.
Books and Other Publications
5Presentations
155Professional Memberships
3Research Projects
2-
Grants-in-Aid for Scientific Research, Japan Society for the Promotion of Science, Apr, 2022 - Mar, 2025
-
Grants-in-Aid for Scientific Research, Japan Society for the Promotion of Science, Apr, 2019 - Mar, 2022