Hiroe Fujita
Shizuoka University
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Featured researches published by Hiroe Fujita.
Physica Scripta | 2016
Hiroe Fujita; Kenta Yuyama; Xiaochun Li; Yuji Hatano; T. Toyama; Masayuki Ohta; Kentaro Ochiai; Naoaki Yoshida; Takumi Chikada; Yasuhisa Oya
Deuterium (D) retention behaviours for 14 MeV neutron irradiated tungsten (W) and fission neutron irradiated W were evaluated by thermal desorption spectroscopy (TDS) to elucidate the correlation between D retention and defect formation by different energy distributions of neutrons in W at the initial stage of fusion reactor operation. These results were compared with that for Fe2+ irradiated W with various damage concentrations. Although dense vacancies and voids within the shallow region near the surface were introduced by Fe2+ irradiation, single vacancies with low concentration were distributed throughout the sample for 14 MeV neutron irradiated W. Only the dislocation loops were introduced by fission neutron irradiation at low neutron fluence. The desorption peak of D for fission neutron irradiated W was concentrated at low temperature region less than 550 K, but that for 14 MeV neutron irradiated W was extended toward the higher temperature side due to D trapping by vacancies. It can be said that the neutron energy distribution could have a large impact on irradiation defect formation and the D retention behaviour.
Fusion Science and Technology | 2017
Shodai Sakurada; Yuki Uemura; Hiroe Fujita; Keisuke Azuma; T. Toyama; Naoaki Yoshida; Tatsuya Hinoki; Sosuke Kondo; Yuji Hatano; Masashi Shimada; Dean A. Buchenauer; Takumi Chikada; Yasuhisa Oya
Abstract The annealing effects on deuterium (D) retention for 0.1–1.0 dpa iron (Fe) ion damaged W were studied as a function of annealing duration. The D2 spectra for Fe damaged W with lower defect concentration showed that D trapped by vacancy clusters was clearly decreased as increasing annealing duration due to the recovery of vacancy clusters. On the other hand, at higher defect concentration, the desorption peak of D trapped by voids was shifted toward higher temperature side, which would be caused by aggregation of vacancies and vacancy clusters. It can be said that the recovery and aggregation behavior of defects are controlled by defect concentration. By disappearing of desorption of D trapped by vacancy clusters after annealing for longer duration, the desorption of D trapped by vacancies was increased, which could be explained by following two possibilities. One is that the retention of hydrogen isotope trapped by monovacancy was increased. The other is that number of vacancies during annihilation process of vacancy cluster were formed by annealing.
Fusion Science and Technology | 2017
Yasuhisa Oya; Cui Hu; Hiroe Fujita; Kenta Yuyama; Shodai Sakurada; Yuki Uemura; S. Masuzaki; Masayuki Tokitani; Miyuki Yajima; Yuji Hatano; Takumi Chikada
Abstract All the hydrogen isotope (H, D, T) simultaneous TDS (Thermal desorption spectroscopy) measurement system (HI-TDS system) was newly designed to evaluate all hydrogen isotope desorption behavior in materials. The present HI-TDS system was operated under Ar purge gas and the H and D desorptions were observed by a quadruple mass spectrometer equipped with an enclosed ion source, although T desorption was evaluated by an ionization chamber or proportional counters. Most of the same TDS spectra for D and T were derived by optimizing the heating rate of 0.5 K s−1 with Ar flow rate of 13.3 sccm. Using this HI-TDS system, D and T desorption behaviors for implanted or DT gas exposed tungsten samples installed in LHD (Large Helical Device) at NIFS (National Institute for Fusion Science) was evaluated. It was found that major hydrogen desorption stages consisted of two temperature regions, namely 700 K and 900 K, which was consistent with the previous hydrogen plasma campaign and most of hydrogen would be trapped by the carbon-dominated mixed-material layer. By implantation, major D desorption was found at ~900 K with a narrow peak due to energetic ion implantation. For gas exposure, H was preferentially replaced by D and T with a lower trapping energy. In addition, T replacement rate by additional H2 gas exposure was evaluated. This fact indicates that the hydrogen replacement mechanism would be clearly changed by exposure methods.
Physica Scripta | 2016
Yasuhisa Oya; Misaki Sato; Xiaochun Li; Kenta Yuyama; Hiroe Fujita; Shodai Sakurada; Yuki Uemura; Yuji Hatano; Naoaki Yoshida; N. Ashikawa; Akio Sagara; Takumi Chikada
Temperature dependence on deuterium (D) retention for He+ implanted tungsten (W) was studied by thermal desorption spectroscopy (TDS) to evaluate the tritium retention behavior in W. The activation energies were evaluated using Hydrogen Isotope Diffusion and Trapping (HIDT) simulation code and found to be 0.55 eV, 0.65 eV, 0.80 eV and 1.00 eV. The heating scenarios clearly control the D retention behavior and, dense and large He bubbles could work as a D diffusion barrier toward the bulk, leading to D retention enhancement at lower temperature of less than 430 K, even if the damage was introduced by He+ implantation. By comparing the D retention for W, W with carbon deposit and tungsten carbide (WC), the dense carbon layer on the surface enhances the dynamic re-emission of D as hydrocarbons, and induces the reduction of D retention. However, by He+ implantation, the D retention was increased for all the samples.
Nuclear materials and energy | 2016
Shodai Sakurada; Kenta Yuyama; Yuki Uemura; Hiroe Fujita; Cui Hu; T. Toyama; N. Yoshida; Tatsuya Hinoki; Sosuke Kondo; Masashi Shimada; Dean A. Buchenauer; Takumi Chikada; Yasuhisa Oya
Nuclear materials and energy | 2016
Takumi Chikada; Teruya Tanaka; Kenta Yuyama; Yuki Uemura; Shodai Sakurada; Hiroe Fujita; Xiaochun Li; K. Isobe; T. Hayashi; Yasuhisa Oya
Fusion Engineering and Design | 2017
Hiroe Fujita; Yuki Uemura; Shodai Sakurada; Keisuke Azuma; Qilai Zhou; T. Toyama; Naoaki Yoshida; Yuji Hatano; Takumi Chikada; Yasuhisa Oya
Journal of Nuclear Materials | 2017
Yuki Uemura; Shodai Sakurada; Hiroe Fujita; Keisuke Azuma; Quilai Zhou; Yuji Hatano; Naoaki Yoshida; H. Watanabe; Makoto Oyaizu; Kanetsugu Isobe; Masashi Shimada; Dean A. Buchenauer; Robert Kolasinski; Takumi Chikada; Yasuhisa Oya
Nuclear materials and energy | 2016
Yasuhisa Oya; Hiroe Fujita; Cui Hu; Yuki Uemura; Shodai Sakurada; Kenta Yuyama; Xiaochun Li; Yuji Hatano; N. Yoshida; H. Watanabe; Y. Nobuta; Yuji Yamauchi; M. Tokitani; S. Masuzaki; Takumi Chikada
Fusion Engineering and Design | 2016
Cui Hu; Hiroe Fujita; Miyuki Yajima; Shodai Sakurada; Yuji Uemura; Keisuke Azuma; Masayuki Tokitani; S. Masuzaki; Naoaki Yoshida; Takumi Chikada; Yasuhisa Oya