C. Fukushima
Toho University
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Featured researches published by C. Fukushima.
Physical Review C | 2007
T. Toshito; K. Kodama; Lembit Sihver; K. Yusa; M. Ozaki; K. Amako; S. Kameoka; K. Murakami; T. Sasaki; S. Aoki; T. Ban; T. Fukuda; M. Komatsu; H. Kubota; N. Naganawa; T. Nakamura; T. Nakano; M. Natsume; K. Niwa; S. Takahashi; J. Yoshida; H. Yoshida; M. Kanazawa; N. Kanematsu; M. Komori; Shinji Sato; M. Asai; T. Koi; C. Fukushima; S. Ogawa
We have studied charged nuclear fragments produced by 200 - 400 MeV/nucleon carbon ions, interacting with water and polycarbonate, using a newly developed emulsion detector. Total and partial charge-changing cross sections for the production of B, Be, and Li fragments were measured and compared with both previously published measurements, and model predictions. This study is of importance for validating and improving carbon ion therapy treatment planning systems, and for estimating the radiological risks for personnel on space missions, since carbon is a significant component of the Galactic Cosmic Rays.
Journal of Instrumentation | 2009
T. Abe; H. Aihara; C Andreop oulos; A. Ankowski; A Badertscher; G. Battistoni; A. Blondel; J. Bouchez; A. Bross; A. Bueno; L. Camilleri; J. E. Campagne; A. Cazes; A. Cervera-Villanueva; G. De Lellis; F. Di Capua; M. Ellis; A. Ereditato; Luigi Salvatore Esposito; C. Fukushima; E.M. Gschwendtner; J.J. Gómez-Cadenas; M. Iwasaki; K. Kaneyuki; Y. Karadzhov; V Kashikhin; Y Kawai; M. Komatsu; E. Kozlovskaya; Y. Kudenko
This report summarises the conclusions from the detector group of the International Scoping Study of a future Neutrino Factory and Super-Beam neutrino facility. The baseline detector options for each possible neutrino beam are defined as follows: 1. A very massive (Megaton) water Cherenkov detector is the baseline option for a sub-GeV Beta Beam and Super Beam facility. 2. There are a number of possibilities for either a Beta Beam or Super Beam (SB) medium energy facility between 1-5 GeV. These include a totally active scintillating detector (TASD), a liquid argon TPC or a water Cherenkov detector. 3. A 100 kton magnetized iron neutrino detector (MIND) is the baseline to detect the wrong sign muon final states (golden channel) at a high energy (20-50 GeV) neutrino factory from muon decay. A 10 kton hybrid neutrino magnetic emulsion cloud chamber detector for wrong sign tau detection (silver channel) is a possible complement to MIND, if one needs to resolve degeneracies that appear in the δ-θ13 parameter space.
Journal of Instrumentation | 2009
T. Abe; H. Aihara; C. Andreopoulos; A. Ankowski; A. Badertscher; G. Battistoni; A. Blondel; J. Bouchez; A. Bross; A. Bueno; L. Camilleri; J. E. Campagne; A. Cazes; A. Cervera-Villanueva; G. De Lellis; F. Di Capua; M. Ellis; A. Ereditato; L. S. Esposito; C. Fukushima; E. Gschwendtner; J.J. Gomez-Cadenas; M. Iwasaki; K. Kaneyuki; Y. Karadzhov; V. Kashikhin; Y. Kawai; M. Komatsu; E. Kozlovskaya; Y. Kudenko
This report summarises the conclusions from the detector group of the International Scoping Study of a future Neutrino Factory and Super-Beam neutrino facility. The baseline detector options for each possible neutrino beam are defined as follows: 1. A very massive (Megaton) water Cherenkov detector is the baseline option for a sub-GeV Beta Beam and Super Beam facility. 2. There are a number of possibilities for either a Beta Beam or Super Beam (SB) medium energy facility between 1-5 GeV. These include a totally active scintillating detector (TASD), a liquid argon TPC or a water Cherenkov detector. 3. A 100 kton magnetized iron neutrino detector (MIND) is the baseline to detect the wrong sign muon final states (golden channel) at a high energy (20-50 GeV) neutrino factory from muon decay. A 10 kton hybrid neutrino magnetic emulsion cloud chamber detector for wrong sign tau detection (silver channel) is a possible complement to MIND, if one needs to resolve degeneracies that appear in the δ-θ13 parameter space.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
T. Toshito; K. Kodama; Ken Yusa; Masanobu Ozaki; K. Amako; S. Kameoka; K. Murakami; T. Sasaki; S. Aoki; T. Ban; T. Fukuda; N. Naganawa; T. Nakamura; M. Natsume; K. Niwa; Satoru Takahashi; M. Kanazawa; Nobuyuki Kanematsu; Masataka Komori; Shinji Sato; Makoto Asai; Tatsumi Koi; C. Fukushima; S. Ogawa; M. Shibasaki; H. Shibuya
Physical Review C | 2008
T. Toshito; K. Kodama; Lembit Sihver; K. Yusa; M. Ozaki; K. Amako; S. Kameoka; K. Murakami; T. Sasaki; S. Aoki; T. Ban; T. Fukuda; H. Kubota; N. Naganawa; T. Nakamura; T. Nakano; M. Natsume; K. Niwa; Satoru Takahashi; J. Yoshida; H. Yoshida; M. Kanazawa; N. Kanematsu; M. Komori; Shinji Sato; M. Asai; T. Koi; C. Fukushima; S. Ogawa; M. Shibasaki
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2008
C. Fukushima; Masashi Kimura; S. Ogawa; H. Shibuya; G. Takahashi; K. Kodama; T. Hara; S. Mikado
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2013
Masashi Kimura; H. Ishida; H. Shibuya; S. Ogawa; T. Matsuo; C. Fukushima; G. Takahashi; Ken’ichi Kuge; Y. Sato; I. Tezuka; S. Mikado
Archive | 2009
N. Agafonova; A. Anokhina; S. Aoki; A. Ariga; T. Ariga; L. Arrabito; D. Autiero; A. Badertscher; A. Bagulya; F. Bersani Greggio; A. Bertolin; M. Besnier; D. Bick; V. V. Boyarkin; C. Bozza; R. Brugnera; Gregorio Antonio Brunetti; S. Buontempo; E. Carrara; A. Cazes; L. Chaussard; M. Chernyavsky; V. Chiarella; N. Chon-Sen; A. Chukanov; M. Cozzi; F. Dal Corso; G. De Lellis; M. De Serio; F. Di Capua