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Pshenichnikov, A.; Kurata, Masaki; Bottomley, D.; Sato, Ikken; Nagae, Yuji; Yamazaki, Saishun
Journal of Nuclear Science and Technology, 57(4), p.370 - 379, 2020/04
Times Cited Count:18 Percentile:68.28(Nuclear Science & Technology)
during severe accidents in boiling water reactorsPshenichnikov, A.; Yamazaki, Saishun; Bottomley, D.; Nagae, Yuji; Kurata, Masaki
Journal of Nuclear Science and Technology, 56(5), p.440 - 453, 2019/05
Times Cited Count:20 Percentile:83.73(Nuclear Science & Technology)Pshenichnikov, A.; Yamazaki, Saishun; Nagae, Yuji; Kurata, Masaki
Proceedings of 27th International Conference on Nuclear Engineering (ICONE-27) (Internet), 8 Pages, 2019/05
Pshenichnikov, A.; Kurata, Masaki; Nagae, Yuji; Yamazaki, Saishun
Proceedings of International Topical Workshop on Fukushima Decommissioning Research (FDR 2019) (Internet), 4 Pages, 2019/05
Yamazaki, Saishun; Pshenichnikov, A.; Pham, V. H.; Nagae, Yuji; Kurata, Masaki; Tokushima, Kazuyuki*; Aomi, Masaki*; Sakamoto, Kan*
Proceedings of Annual Topical Meeting on Reactor Fuel Performance (TopFuel 2018) (Internet), 8 Pages, 2018/10
It is predictively evaluated that degradation of fuel assembly proceeded in a certain steam-starved condition at the early stage of a SA at 1F unit 2 (BWR). As for PWR fuel assembly, effective steam flow rate was properly indicated by normalizing to a unit of g-H
O/sec/rod which is used as an important parameter for evaluating fuel degradation progression. Due to the inhomogeneous configuration of BWR fuel assembly, the difference of Zry oxidation and hydrogen uptake between the inside and outside of the channel box cannot be properly evaluated by this normalization. Instead of g-H
O/sec/rod, proper evaluation unit for BWR configuration is necessary. To accumulate Zry oxidation and hydrogen uptake data for steam-starved conditions, high temperature oxidation tests were performed using a simulated BWR fuel bundle sample. The use of equivalent diameter of the cross section of BWR fuel assembly was proposed for normalization of effective steam flow rate.
Oguri, Hidetomo; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Yamazaki, Saishun; Takagi, Akira*; Koizumi, Isao; Ueno, Akira
JPS Conference Proceedings (Internet), 8, p.011009_1 - 011009_6, 2015/09
ion sourceUeno, Akira; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Takagi, Akira*; Yamazaki, Saishun; Oguri, Hidetomo
AIP Conference Proceedings 1655, p.030010_1 - 030010_7, 2015/04
Times Cited Count:5 Percentile:81.33(Physics, Applied)The J-PARC cesiated rf-driven H
ion source was successfully developed to satisfy the J-PARC second stage requirements of an H
ion beam of 60mA within normalized emittances of 1.5
mm
mrad both horizontally and vertically, a flat top beam duty factor of 1.25
and a life-time of longer than 1 month. In the source, the rod-filter-field effect was successfully tuned to produce the necessary beam with about 20
lower 2MHz rf-power by a newly devised method of the center-gapped rod-filter-magnets last year. In this paper, the rod-filter-filed optimization by using the trippel-gaps (TG) and two different cross-sections (RFM1:4.75mm
10mm and RFM2:5mm
10mm) of rod-filter-magnets are presented. With both of RFM1 and RFM2, the optimum rod-filter effect was produced with the gaps of around 2mm. However, it takes 5 times longer period to condition the source to produce the necessary beam with RFM2 compared with RFM1.
ion sourceUeno, Akira; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Takagi, Akira*; Yamazaki, Saishun; Oguri, Hidetomo
AIP Conference Proceedings 1655, p.030008_1 - 030008_10, 2015/04
Times Cited Count:7 Percentile:87.33(Physics, Applied)To satisfy the J-PARC second stage requirements of an H
ion beam of 60 mA within normalized emittances of 1.5
mm
mrad both horizontally and vertically, a flat top beam duty factor of 1.25% and a life-time of longer than 1 month, the J-PARC cesiated rf-driven H
ion source was developed by using an internal-antenna developed at the SNS. The maintenance and operation procedure to minimize the source replacement time on the beam line, which maximizes the J-PARC beam time, is presented. The Ar filled source after the pre-conditioning to produce the required beam at a test-stand successfully produced the required beam on the beam line within 8 hours. The feedback controls of 2 MHz rf-matching and an H
ion beam intensity are also presented. The rf-matching feedback by using two vacuum variable capacitors produced almost perfect matching. The H
ion beam intensity was controlled within errors of
0.1 mA by the rf-power feedback.
Kondo, Yasuhiro; Morishita, Takatoshi; Yamazaki, Saishun; Hori, Toshihiko; Sawabe, Yuki; Chishiro, Etsuji; Fukuda, Shimpei; Hasegawa, Kazuo; Hirano, Koichiro; Kikuzawa, Nobuhiro; et al.
Physical Review Special Topics; Accelerators and Beams, 17(12), p.120101_1 - 120101_8, 2014/12
Times Cited Count:8 Percentile:43.61(Physics, Nuclear)We performed a beam test of a new radio frequency quadrupole linac (RFQ III) for the beam current upgrade of the Japan Proton Accelerator Research Complex. First, the conditioning of RFQ III was conducted, and after 20 h of conditioning, RFQ III became very stable with a nominal peak power and duty factor of 400 kW and 1.5%, respectively. An off-line beam test was subsequently conducted before installation in the accelerator tunnel. The transmission, transverse emittance, and energy spread of the 50-mA negative hydrogen beam from RFQ III were measured and compared with simulation results. The experiment and simulation results showed good agreement; therefore, we conclude that the performance of RFQ III conforms to its design.
Kondo, Yasuhiro; Morishita, Takatoshi; Yamazaki, Saishun; Hori, Toshihiko; Sawabe, Yuki; Takagi, Akira*
Proceedings of 27th International Linear Accelerator Conference (LINAC 2014) (Internet), p.267 - 269, 2014/12
We performed a beam test of a new 324-MHz 3-MeV H
RFQ (RFQ III) for the beam-current upgrade of the J-PARC linac. RFQ III is the first RFQ developed to meet the requirement of the J-PARC linac. The peak beam current is 50 mA, pulse length is 500 micro-sec, and the repetition is 25 Hz. Prior to the installation to the accelerator tunnel in summer of 2014, we constructed a test stand for off line testing of the new ion source and RFQ. Basic performances of RFQ III such as transmission and emittances were measured. In this paper, the beam test results are presented.
Oguri, Hidetomo; Hasegawa, Kazuo; Ito, Takashi; Chishiro, Etsuji; Hirano, Koichiro; Morishita, Takatoshi; Shinozaki, Shinichi; Ao, Hiroyuki; Okoshi, Kiyonori; Kondo, Yasuhiro; et al.
Proceedings of 11th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.389 - 393, 2014/10
no abstracts in English
ion source for the J-PARCKoizumi, Isao; Ueno, Akira; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Takagi, Akira*; Yamazaki, Saishun; Oguri, Hidetomo
Proceedings of 10th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.920 - 923, 2014/06
In order to satisfy the J-PARC (Japan Proton Accelerator Research Complex) 2nd stage requirements the J-PARC rf-driven H
ion source is under development. The source plasma is produced by an about 50 W CW 30 MHz-rf and an about 40 kW pulsed 2 MHz-rf. The Cs is installed into the plasma chamber by opening the Cs-valve between the plasma chamber and the Cs oven, which is heated to 200
240
C. The H
ion beam current is maximized by optimizing the Cs quantity depending upon the Cs-valve opening time, the PE temperature depending upon the flow rate of the air through the PE cooling plate, the AMFC by the AMFC coil current, and so on. The experimental results using the plasma chamber made of copper, which satisfied the above requirements, were reported last year. The experimental results using the plasma chamber made of stainless steel are presented in this paper. The observed several interesting differences between the two plasma chambers are also presented.
Okoshi, Kiyonori; Ikegami, Kiyoshi*; Koizumi, Isao; Ueno, Akira; Takagi, Akira*; Yamazaki, Saishun; Oguri, Hidetomo
Proceedings of 10th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.946 - 949, 2014/06
A J-PARC ion source driven with a LaB6 filament is being operated without any serious trouble since the restoration from the earthquake. The H
ion current from the source is routinely restricted 19 mA for the filament lifetime. In order to increase the beam power at the linac beam operation, the beam current from the ion source was increased to 22 mA. At this operation, the filament lifetime was estimated by the reduction in the filament current. According to the steep reduction in the filament current, the break of the filament was predicted. Although the filament has broken after 10 h from the steep current reduction, the beam operation was restarted 8 h later by the preparation for the exchange of new filament. At the study time for the 3 GeV synchrotron, the ion source was operated at 30 mA for 8 days.
ion sourceUeno, Akira; Koizumi, Isao; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Takagi, Akira*; Yamazaki, Saishun; Oguri, Hidetomo
Review of Scientific Instruments, 85(2), p.02B133_1 - 02B133_5, 2014/02
Times Cited Count:6 Percentile:26.12(Instruments & Instrumentation)no abstracts in English
ion source for the J-PARCYamazaki, Saishun; Ueno, Akira; Namekawa, Yuya*; Okoshi, Kiyonori; Ikegami, Kiyoshi*; Takagi, Akira*; Koizumi, Isao; Oguri, Hidetomo
Proceedings of 9th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.260 - 264, 2013/08
A cesium (Cs) seeded RF-driven H
ion source using an internal-antenna developed at the SNS (Spallation Neutron Source) is under development for the J-PARC (Japan Proton Accelerator Research Complex). The axial magnetic field optimization by using an axial magnetic field compensation (AMFC) coil significantly enhances the H
ion beam by typically 10%. An H
ion beam with a flat top duty factor of 2.5% (1 ms
25 Hz) of 77 mA, whose about 90% (corresponding to about 70 mA) of emittance of each direction is within 1.5
mm
mrad, is successfully extracted. During a demonstration operation over 100-hours, an H
ion beam over 66 mA was successfully produced with a relatively low RF power of about 40 kW by seeding Cs for 4-minutes a day.
Oguri, Hidetomo; Ikegami, Kiyoshi*; Okoshi, Kiyonori; Koizumi, Isao; Takagi, Akira*; Namekawa, Yuya*; Yamazaki, Saishun; Ueno, Akira
Proceedings of 9th Annual Meeting of Particle Accelerator Society of Japan (Internet), p.1081 - 1083, 2013/08
no abstracts in English
Oguri, Hidetomo; Ikegami, Kiyoshi*; Okoshi, Kiyonori; Koizumi, Isao; Namekawa, Yuya*; Ueno, Akira; Takagi, Akira*; Yamazaki, Saishun
AIP Conference Proceedings 1515, p.379 - 385, 2013/02
Times Cited Count:4 Percentile:81.46(Physics, Applied)The J-PARC was extensively damaged by the earthquake in March 2011. The ion source had some damages such as dew condensation on the ion source surface due to the flooding in the accelerator tunnel, vacuum leakage due to the breaking of the viewing port and vacuum pump failure due to the strong quake. The restoration work was accomplished on schedule, and the linac beam operation was restarted in December 9th. The ion source supplies the beam to the accelerator without serious aftereffects of the earthquake. Availability of the ion source is one of the important issues because it is directly related to the operation time of the J-PARC. To evaluate the lifetime of the present ion source, we started 2 months beam operation. The results of recent four beam runs show the ion source is capable of continuous operation for approximately 1,200 hours with the beam current of 17 mA. For another attempt to enhance the ion source availability, we tried to decrease the time for maintenance to replace consumable elements. By unitizing the replacement elements and keeping them under the vacuum condition until just before the installing, the maintenance is completed within 24 hours without any beam performance degradation of the ion source.
ion source for the J-PARCUeno, Akira; Namekawa, Yuya*; Yamazaki, Saishun; Okoshi, Kiyonori; Koizumi, Isao; Ikegami, Kiyoshi*; Takagi, Akira*; Oguri, Hidetomo
AIP Conference Proceedings 1515, p.331 - 340, 2013/00
Times Cited Count:9 Percentile:92.79(Physics, Applied)In order to satisfy the J-PARC second stage requirements of an H
ion beam current of 60 mA within normalized emittances of 1.5
-mm-mrad both horizontally and vertically, a flat top beam duty factor of 1.25% (500 micros
25 Hz) and a life-time of more than 50 days, a cesiated RF-driven H
ion source using a internal-antenna developed at the Spallation Neutron Source (SNS) was developed. The J-PARC RF-driven source was manufactured by modifying the J-PARC cesiated H
ion source driven with two tungsten (W) filaments, which successfully produced a 76.2 mA H
ion beam current but had an insufficient life time of about 500 hours. It successfully produced a 77.5 mA H
ion beam with a flat top duty factor of 2% (800 micros
25 Hz) whose 87.7% (68 mA) and 89.1% (69 mA) are within horizontal and vertical 1.5
-mm-mrad emittances, respectively. It also had successfully produced more than 60 mA within 1.5
-mm-mrad emittances H
ion beam continuously over 100 hours.
ion sourceUeno, Akira; Namekawa, Yuya*; Yamazaki, Saishun; Okoshi, Kiyonori; Koizumi, Isao; Ikegami, Kiyoshi*; Takagi, Akira*; Oguri, Hidetomo
AIP Conference Proceedings 1515, p.409 - 416, 2013/00
Times Cited Count:7 Percentile:90.09(Physics, Applied)In order to satisfy the J-PARC second stage requirements a cesiated RF-driven H
ion source using a internal-antenna developed at the Spallation Neutron Source (SNS) was developed. As similar as the SNS ion source, two matching networks for pulsed high-temperature 2MHz-RF plasma and CW low-temperature 30MHz-RF plasma are used. Each of them is composed of two vacuum variable condensers (VVCs). In order to supply pulsed 60kW - 2MHz-RF power from the power supply (PS) on the ground level, a one-turn isolation transformer using FINEMET cores is installed between the PS and the J-PARC ion source. Up to 46kW of pulsed 2MHz-RF power is successfully input to the plasma stably and with almost no reflected power.
Yamazaki, Saishun*; Ouchi, Atsushi*; Sakamoto, Kan*; Sato, Takumi; Ogata, Takanari*; Yamano, Hidemasa
no journal, ,
The thickness reduction rate of Fe/stainless steel by eutectic reaction with U/U-Zr alloys was estimated in order to provide the basis for developing between the fuel and cladding eutectic reaction phenomenon during core disruptive accidents (CDA) in metal-fueled sodium-cooled fast reactors. In the case of the intervention of eutectic melt expected during CDA, the thickness reduction rate of Fe/stainless steel for fuel-cladding material has slowed.