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-gas exposure at high temperaturesTakeda, Yusuke; Iida, Kiyoshi*; Sato, Shinji*; Matsuo, Tadatoshi*; Nagashima, Yasuyuki*; Okubo, Nariaki; Kondo, Keietsu; Hirade, Tetsuya
JPS Conference Proceedings (Internet), 25, p.011023_1 - 011023_3, 2019/03
In this study, we prepared samples under two different conditions, (1) 810
C, for 600 min, and (2) 850C, for 720 min. A depth-profile analysis of the surfaces of the samples is conducted through Doppler broadening (DB) measurements of positron annihilation 
rays using a slow positron beam. It was indicated that many of positrons annihilated in defects near the surface. According to the TEM image, there are nano-crystal grains near the surface and then positrons can diffuse in the grains and annihilate in defects at the grain boundaries. Furthermore, DB measurements indicated that there is a depth dependence on the chemical composition where positrons annihilate. EDS spectroscopy measurements also indicated that there is a depth dependence of impurities such as Vanadium. These results indicated change of the chemical composition at the grain boundaries.
Hirade, Tetsuya
JPS Conference Proceedings (Internet), 25, p.011021_1 - 011021_2, 2019/03
Irradiation of water produce some reactive species such as OH radical. OH is formed by the reaction of a water cation and a water molecule just after ionization. On the other hand, a high energy positron injected in water will form cations and excess electrons even at the end part of the track. And hence, some positrons can form Positronium (Ps) with one of the excess electrons. The electrons in OH and Ps used to be in a same orbital in a water molecule before ionization of that water molecule. Therefore they were singlet at the time of the ionization. Every electron have each own hyperfine coupling constant after ionization. In water, reaction between Ps and OH, such as radical reaction or spin conversion, is possible. Therefore, quantum beats on these reaction can occur and the frequency of quantum beats will indicate the hyperfine coupling constant of OH which depends on the structure around OH. Therefore it is becoming possible to discuss the structure of water and reactivity of OH in the structure.
Watanabe, Masao; Nojiri, Hiroyuki*; Ito, Shinichi*; Kawamura, Seiko; Kihara, Takumi*; Masuda, Takatsugu*; Sahara, Takuro*; Soda, Minoru*; Takahashi, Ryuta
JPS Conference Proceedings (Internet), 25, p.011024_1 - 011024_5, 2019/03
Recently, neutron scattering experiments have been rapidly progressed under high magnetic field. In the J-PARC, proto-type compact pulse magnet system with the power supply, the coil and the sample stick has been developed. Basic specifications of the power supply are as follows; maximum charged voltage with capacitor is 2 kV, maximum current is 8 kA, repetition rate is a pulse per several minutes and pulse duration is several msec. Maximum magnetic field in the coil is more than 30 Tesla. The sample stick is designed for Orange-Cryostat. In this presentation, We report the details of the pulsed magnet system and the performance of it on neutron scattering experiments at MLF beam line (HRC).
Otani, Masashi*; Kondo, Yasuhiro; Saito, Naohito; Hasegawa, Kazuo; 7 of others*; J-PARC E34 Collaboration*
JPS Conference Proceedings (Internet), 25, p.011027_1 - 011027_5, 2019/03
We are developing a linac dedicated to the muon acceleration. It enables us to measure the muon anomalous magnetic moment with an accuracy of 0.1 ppm and search for electric dipole moment with a sensitivity of 10
cm to explore beyond Standard Model of elementary particle physics. As a first step for demonstration of the muon acceleration, we are developing the source of slow muon with which RFQ acceleration is conducted. This paper describes status of these developments.
Kondo, Yasuhiro; Morishita, Takatoshi
JPS Conference Proceedings (Internet), 25, p.011030_1 - 011030_5, 2019/03
In this paper, we present the performance and RFQs at J-PARC. In the summer of 2014, we replaced the frontend system of the J-PARC linac for beam current upgrade. An RF driven ion source (IS) and a radio frequency quadrupole linac (RFQ III) are newly developed to make the linac be capable for 50 mA peak current operation. Prior to the installation to the accelerator tunnel, we conducted an off-line beam test at an RFQ test stand, and confirmed the basic performance of the IS and RFQ as their design. The 50 mA peak current was demonstrated at this test stand and we also succeeded the 50 mA operation in the actual linac. The used RFQ (RFQ I) replaced by RFQ III will be used for beam test of laser charge exchange system for the ADS project and beam scraper and so on. The other RFQ developed as a spare of RFQ I will be used for world first muon acceleration experiment. The status of these RFQs is also shown.
Osakabe, Toyotaka; Kuwahara, Keitaro*; Honmoto, Satoru*; Kato, Yoshihiro*
no journal, ,
no abstracts in English
Kaneko, Koji; Matsuda, Masaaki*; Tsutsui, Satoshi; Cheung, Y. W.*; Hu, Y. J.*; Goh, S. K.*; Matsumoto, Takuya*; Imai, Masaki; Tanioku, Yasuaki*; Kanagawa, Hibiki*; et al.
no journal, ,
no abstracts in English
