Ishibashi Y.

Ishida S.

Itoh M.

Karasudani K.

Kasamatsu K.

Matsuda Y.

Nasu Y.

Okamoto J.

Tanaka K.

Yoshioka R.

English

紀要類（bulletin）departmental bulletin pape

Ishibashi, Y.

Itoh, M.

Matsuda, Y.

Tanaka, K.

Nasu, Y.

Okamoto, J.

Karasudani, K.

Yoshioka, R.

Ishida, S.

Kasamatsu, K.

Tohoku University Repository (TOUR) / 東北大学機関リポジトリ

Development of Neutron/Ion Irradiation System著者 Ishibashi Y., Itoh M.  Matsuda Y., Tanaka K.,Nasu Y., Okamoto J., Karasudani K., YoshiokaR., Ishida S., Kasamatsu K.journal orpublication titleCYRIC annual reportvolume 2016-2017page range 57-58year 2017URL http://hdl.handle.net/10097/0012806057  CYRIC Annual Report 2016-2017    II. 10.  Development of Neutron/Ion Irradiation System    Ishibashi Y., Itoh M., Matsuda Y., Tanaka K., Nasu Y., Okamoto J., Karasudani K.,  Yoshioka R., Ishida S., and Kasamatsu K.  Cyclotron and Radioisotope Center, Tohoku University   * New fundamental technologies which control quantum particles such as neutron, muon, radioactive nuclei, etc., are developed to provide the safety infrastructure for the super smart society (Society 5.0). Neutron/ion irradiation experiments are performed using the 930AVF cyclotron in CYRIC to evaluate soft errors of semiconductor devices which are used for Internet of Things (IoT). Table 1 shows the operation time of the AVF cyclotron by the beam, and the ratio is shown in Fig. 1. Table 2 lists the ion nuclides which can be supplied by the cocktail beam acceleration technique in CYRIC. These beams can be switched without changing the magnetic field of the AVF cyclotron. Cocktail beam irradiation experiments occupied about half of the irradiation beam time. In cocktail beam experiments, many users apply several ion beams to change the LET. In order for users to take a longer irradiation time in the limited beam time, we need to switch the beam quickly. In the present status, flux measurements take long time to adjust the flux to the required one. Previously, for the flux measurements, we have used a Si detector located at the irradiation position (downstream of the vacuum window). In this method, it was necessary to enter the experimental room several times for installing a Si detector and removing it after the flux adjustment. In order to reduce these times, we installed a Si detector in the beam line and attached it to a remotely controllable ladder which can be inserted and removed from the beam line. Because this detector was located upstream of beam irradiation position, it was necessary to calibrate the actual flux by comparing with the flux of the beam at the irradiation position. Then, the detector once calibrated, flux adjustment was possible without entering the experimental room unless the beam nuclide changes. However, the Si detector deteriorated rapidly due to the radiation damage. In addition, in the case of a high intensity beam (more than 103 particles/s/cm2) irradiation, it was 58  necessary to attach a collimator in order to reduce the number of beam particles which hit the detector to less than 103 particles/s.  In order to solve the problem, we installed plastic scintillation detectors instead of the Si detectors. The plastic scintillators are more resistant to the radiation damage than the Si detector. These improvements shortened the time of the flux measurement, and increase the irradiation time in the limited beam time.  Table 1. Irradiation time for each beam nuclide.  Proton Neutron Cocktail beam FY2016 (2016/05 ~ 2017/03) 91 h 148 h 273 h FY2017 (2017/05 ~ 2018/03) 0 h 185 h 182 h Total 91 h 333 h 455 h  Table 2. Ion nuclides of cocktail beams that can be supplied in CYRIC. Ion nuclides Energy [MeV] LET(Si)[MeV/mg/cm2] 15N3+ 56.3 3.3 20Ne4+ 75 6.3 40Ar8+ 150 15.3 84Kr17+ 322.5 39.9 129Xe25+ 454.2 69.2     Figure 1.  Ratio of the beam time of irradiation nuclides. 

Development of Neutron/Ion Irradiation System

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Development of Neutron/Ion Irradiation System

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