Saku Mochizuki
Waseda University
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Publication
Featured researches published by Saku Mochizuki.
Journal of Instrumentation | 2017
J. Kataoka; A. Kishimoto; Leo Tagawa; Saku Mochizuki; Toshiyuki Toshito; Masashi Kimura; Yuto Nagao; Keisuke Kurita; Mitsutaka Yamaguchi; Naoki Kawachi
Particle therapy is an advanced cancer therapy that uses a feature known as the Bragg peak, in which particle beams suddenly lose their energy near the end of their range. The Bragg peak enables particle beams to damage tumors effectively. To achieve precise therapy, the demand for accurate and quantitative imaging of the beam irradiation region or dosage during therapy has increased. The most common method of particle range verification is imaging of annihilation gamma rays by positron emission tomography. Not only 511-keV gamma rays but also prompt gamma rays are generated during therapy; therefore, the Compton camera is expected to be used as an on-line monitor for particle therapy, as it can image these gamma rays in real time. Proton therapy, one of the most common particle therapies, uses a proton beam of approximately 200 MeV, which has a range of ~ 25 cm in water. As gamma rays are emitted along the path of the proton beam, quantitative evaluation of the reconstructed images of diffuse sources becomes crucial, but it is far from being fully developed for Compton camera imaging at present. In this study, we first quantitatively evaluated reconstructed Compton camera images of uniformly distributed diffuse sources, and then confirmed that our Compton camera obtained 3 %(1 σ) and 5 %(1 σ) uniformity for line and plane sources, respectively. Based on this quantitative study, we demonstrated on-line gamma imaging during proton irradiation. Through these studies, we show that the Compton camera is suitable for future use as an on-line monitor for particle therapy.
Scientific Reports | 2017
A. Kishimoto; J. Kataoka; Leo Tagawa; Saku Mochizuki; Shinji Ohsuka; Yuto Nagao; Keisuke Kurita; Mitsutaka Yamaguchi; Naoki Kawachi; Keiko Matsunaga; Hayato Ikeda; Eku Shimosegawa; Jun Hatazawa
In the field of nuclear medicine, single photon emission tomography and positron emission tomography are the two most common techniques in molecular imaging, but the available radioactive tracers have been limited either by energy range or difficulties in production and delivery. Thus, the use of a Compton camera, which features gamma-ray imaging of arbitrary energies from a few hundred keV to more than MeV, is eagerly awaited along with potential new tracers which have never been used in current modalities. In this paper, we developed an ultra-compact Compton camera that weighs only 580 g. The camera consists of fine-pixelized Ce-doped Gd3Al2Ga3O12 scintillators coupled with multi-pixel photon counter arrays. We first investigated the 3-D imaging capability of our camera system for a diffuse source of a planar geometry, and then conducted small animal imaging as pre-clinical evaluation. For the first time, we successfully carried out the 3-D color imaging of a live mouse in just 2 h. By using tri-color gamma-ray fusion images, we confirmed that 131I, 85Sr, and 65Zn can be new tracers that concentrate in each target organ.
Journal of Instrumentation | 2017
Saku Mochizuki; J. Kataoka; Leo Tagawa; Yasuhiro Iwamoto; Hiroshi Okochi; N. Katsumi; S. Kinno; Makoto Arimoto; Takuya Maruhashi; K. Fujieda; T. Kurihara; Shinji Ohsuka
Considerable amounts of radioactive substances (mainly 137Cs and 134Cs) were released into the environment after the Japanese nuclear disaster in 2011. Some restrictions on residence areas were lifted in April 2017, owing to the successive and effective decontamination operations. However, the distribution of radioactive substances in vast areas of mountain, forest and satoyama close to the city is still unknown; thus, decontamination operations in such areas are being hampered. In this paper, we report on the first aerial gamma-ray imaging of a schoolyard in Fukushima using a drone that carries a high sensitivity Compton camera. We show that the distribution of 137Cs in regions with a diameter of several tens to a hundred meters can be imaged with a typical resolution of 2–5 m within a 10–20 min flights duration. The aerial gamma-ray images taken 10 m and 20 m above the ground are qualitatively consistent with a dose map reconstructed from the ground-based measurements using a survey meter. Although further quantification is needed for the distance and air-absorption corrections to derive in situ dose map, such an aerial drone system can reduce measurement time by a factor of ten and is suitable for place where ground-based measurement are difficult.
Scientific Reports | 2018
A. Koide; J. Kataoka; Takamitsu Masuda; Saku Mochizuki; Koki Sueoka; Leo Tagawa; K. Fujieda; Takuya Maruhashi; Takuya Kurihara; Taku Inaniwa
Imaging of nuclear gamma-ray lines in the 1–10 MeV range is far from being established in both medical and physical applications. In proton therapy, 4.4 MeV gamma rays are emitted from the excited nucleus of either 12C* or 11B* and are considered good indicators of dose delivery and/or range verification. Further, in gamma-ray astronomy, 4.4 MeV gamma rays are produced by cosmic ray interactions in the interstellar medium, and can thus be used to probe nucleothynthesis in the universe. In this paper, we present a high-precision image of 4.4 MeV gamma rays taken by newly developed 3-D position sensitive Compton camera (3D-PSCC). To mimic the situation in proton therapy, we first irradiated water, PMMA and Ca(OH)2 with a 70 MeV proton beam, then we identified various nuclear lines with the HPGe detector. The 4.4 MeV gamma rays constitute a broad peak, including single and double escape peaks. Thus, by setting an energy window of 3D-PSCC from 3 to 5 MeV, we show that a gamma ray image sharply concentrates near the Bragg peak, as expected from the minimum energy threshold and sharp peak profile in the cross section of 12C(p,p)12C*.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
A. Koide; J. Kataoka; Yasuhiro Iwamoto; Koki Sueoka; Saku Mochizuki; Makoto Arimoto; Taku Inaniwa
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
J. Kataoka; A. Kishimoto; Saku Mochizuki; Leo Tagawa; A. Koide; Koki Sueoka; Hayato Morita; Takuya Maruhashi; K. Fujieda; T. Kurihara; Makoto Arimoto; Hiroshi Okochi; N. Katsumi; S. Kinno; Keiko Matsunaga; Hayato Ikeda; Eku Shimosegawa; Jun Hatazawa; Shinji Ohsuka; Toshiyuki Toshito; Masashi Kimura; Yuto Nagao; Mitsutaka Yamaguchi; Keisuke Kurita; Naoki Kawachi
The Japan Society of Applied Physics | 2018
Leo Tagawa; J. Kataoka; Koki Sueoka; Kazuya Fuzieda; Takuya Kurihara; Makoto Arimoto; Saku Mochizuki; Takuya Maruhashi; Toshiyuki Toshito; Mitsuhiro Kimura; Taku Inaniwa
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
Leo Tagawa; J. Kataoka; Koki Sueoka; K. Fujieda; T. Kurihara; Makoto Arimoto; Saku Mochizuki; T. Maruhash; Toshiyuki Toshito; Masashi Kimura; Taku Inaniwa
The Japan Society of Applied Physics | 2017
A. Kishimoto; J. Kataoka; Leo Tagawa; Saku Mochizuki; Shinji Ohsuka; Keiko Matsunaga; Hayato Ikeda; Eku Shimosegawa; Jun Hatazawa; Naoki Kawachi; Yuto Nagao; Mitsutaka Yamaguchi; Keisuke Kurita
The Japan Society of Applied Physics | 2017
Yasuhiro Iwamoto; J. Kataoka; Leo Tagawa; Saku Mochizuki; Hiroshi Okochi; Naoya Katsumi; Shuntaro Kinno; Shinji Ohsuka