T. Fujita
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
T. Fujita has a total of 16 co-authors. Here are the top co-authors by number of shared publications:
- H. Okada
Institute of Advanced Energy, Kyoto University 2 , Kyoto 606-8501
1 shared publication - Heishun Zen
Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Kyoto, Japan
1 shared publication - Hideaki Ohgaki
Institute of Advanced Energy, Kyoto University, Gokasho, Uji 611-0011, Kyoto, Japan
1 shared publication - Kazunobu Nagasaki
Kyoto University
1 shared publication - Kenichi Nagaoka
National Institute for Fusion Science, National Institutes of Natural Sciences, Toki, Japan
1 shared publication - R. Yamato
Graduate School of Energy Science, Kyoto University 1 , Kyoto 606-8501
1 shared publication
Latest Publications
- 1 March 2025
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 96 (3)
Measurement of x-ray bremsstrahlung radiation from high energy electrons by stochastic acceleration in Heliotron J
A synthetic diagnostic of x-ray bremsstrahlung radiation and a Monte Carlo radiation transport simulation were carried out to obtain the electron energy distribution in stochastic acceleration experiments in Heliotron J, a mid-sized heliotron-type magnetic confinement device. Three sets of LaBr3(Ce) scintillator and photomultiplier tubes were installed in Heliotron J in three directions relative to the magnetic field line, co, counter, and perpendicular, to determine the velocity distribution of the high-energy electrons. These systems are positioned about 5 m away from the vacuum chamber and shielded by lead blocks and magnetic shields to reduce the influence of stray radiation and magnetic fields. The vacuum chamber of Heliotron J is made of stainless steel with a 3D helical shape. Since its x-ray shielding effect is not negligible when obtaining the x-ray energy distribution in the vacuum chamber, the Monte Carlo radiation transport code particle and heavy ion transport code system was applied to Heliotron J to clarify the shielding effect. Given the vacuum chamber and coil shape information and x-ray energy distribution expected in the vacuum chamber, this code can calculate x-ray energy distribution considering the shielding effect of Heliotron J. This simulation model was based on computer aided design data of Heliotron J devices. The x-ray energy distribution in the vacuum vessel was adapted until the simulated and measured x-ray spectra outside the vacuum vessel match with each other. The shapes of resultant distribution have two types of shape: power-law distribution at more than 450 keV and Maxwell distribution at less than 450 keV. At a higher energy range, x-ray bremsstrahlung energy distribution is consistent with the characteristic of stochastic acceleration.
- 1 March 2025
- Published by AIP Publishing in Review of Scientific Instruments
- Vol. 96 (3)
Measurement of x-ray bremsstrahlung radiation from high energy electrons by stochastic acceleration in Heliotron J
A synthetic diagnostic of x-ray bremsstrahlung radiation and a Monte Carlo radiation transport simulation were carried out to obtain the electron energy distribution in stochastic acceleration experiments in Heliotron J, a mid-sized heliotron-type magnetic confinement device. Three sets of LaBr3(Ce) scintillator and photomultiplier tubes were installed in Heliotron J in three directions relative to the magnetic field line, co, counter, and perpendicular, to determine the velocity distribution of the high-energy electrons. These systems are positioned about 5 m away from the vacuum chamber and shielded by lead blocks and magnetic shields to reduce the influence of stray radiation and magnetic fields. The vacuum chamber of Heliotron J is made of stainless steel with a 3D helical shape. Since its x-ray shielding effect is not negligible when obtaining the x-ray energy distribution in the vacuum chamber, the Monte Carlo radiation transport code particle and heavy ion transport code system was applied to Heliotron J to clarify the shielding effect. Given the vacuum chamber and coil shape information and x-ray energy distribution expected in the vacuum chamber, this code can calculate x-ray energy distribution considering the shielding effect of Heliotron J. This simulation model was based on computer aided design data of Heliotron J devices. The x-ray energy distribution in the vacuum vessel was adapted until the simulated and measured x-ray spectra outside the vacuum vessel match with each other. The shapes of resultant distribution have two types of shape: power-law distribution at more than 450 keV and Maxwell distribution at less than 450 keV. At a higher energy range, x-ray bremsstrahlung energy distribution is consistent with the characteristic of stochastic acceleration.