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RECENT STATUS OF NEUTRON AND GAMMA-RAY MEASUREMENTS FOR DIAGNOSTICS IN JAPAN Kentaro OCHIAI JAPAN ATOMIC ENERGY AGENCY FNS.

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Presentation on theme: "RECENT STATUS OF NEUTRON AND GAMMA-RAY MEASUREMENTS FOR DIAGNOSTICS IN JAPAN Kentaro OCHIAI JAPAN ATOMIC ENERGY AGENCY FNS."— Presentation transcript:

1 RECENT STATUS OF NEUTRON AND GAMMA-RAY MEASUREMENTS FOR DIAGNOSTICS IN JAPAN Kentaro OCHIAI JAPAN ATOMIC ENERGY AGENCY FNS

2 OUTLINE  Neutron measurement in JAEA/FNS Triplet coincidence TOF spectrometer Double crystal TOF spectrometer (Sasao) PPAC instruments Flash ADC system (Ishikawa) Stilbene detector (Ishikawa) Cherenkov detector (V.Yury)  Gamma-ray measurement for fast ions in JAEA/FNS D( ,  ) 6 Li gamma-ray Activation method for leakage a particle

3 FNS Triplet coincidence spectrometer Some experiment of neutron spectroscopy is currently carried out in Japan (JAEA/FNS). In order to measure tritium burning ratio (DD/DT) and high resolution neutron spectrum, JAEA/FNS and Naogoya Univ. has conducted the triplet coincidence spectroscopy Principle of triplet coincidence methodApparatus of coincident measurement

4 FNS Result and Future works N. Naoi et al. ( Nagoya university ) will present the study on HTPD2006 May. 2006 We have obtained the energy resolution within 6% using triplet coincidence. In order to obtain the resolution within 2.5%, Some improvement will be done.

5 FNS Double crystal TOF spctroscopy First Detector Second Detector Prof. M. Sasao will mention the detail of the experiment. So, here the present status of second detector for JT-60 diagnostics are presented.

6 FNS Result of second detector property We obtained the TOF spectrum the second detector using by 9 Be-d neutron. The efficiency, resolution and gamma effect will be obtained near D-D neutron energy. Gamma-flash (time~0sec) 4.16-MeV neutron 0.9-MeV neutron Gamma 3.44-MeV neutron Neutron spectrum of second detector using by 9 Be-d neutrons 2.22 and 2.59-MeV

7 FNS PPAC instruments Experiment on an AVF-cyclotron in Tohoku-Univ. Research of rise time of Parallel Plate Avalanche Counter (PPAC) is conducted using by heavy ion beam (AVF- Cyclotoron in Tohoku-Univ.)

8 FNS Result (PPAC) We obtained the rise time within 3nsec. Some improvement is needed to be within 1 nsec

9 FNS D(,) 6 Li 2.18MeV gamma-ray ITER D-T plasma ~ 500m 3  5 x 10 11 photon/sec Target C 2 D 2 Kobe university Tandem Van de Graaff accelerator, Pelletron 5SDH-2, +15 line Nuclear properties of D( ,  ) 6 Li 2.18MeV gamma-ray was researched due to the diagnostics of high energetic  -particle.

10 FNS Result (D(,) 6 Li 2.18MeV gamma-ray) We obviously obtained the photo peak of the gamma and energy dependence. It was found that energy dependency was different from the past data. Photo peak of D(a,g)6Li 2.18MeV gamma-ray Energy dependency of gamma yield

11 FNS Activation method for lost  particle Irradiated CaF 2 sample 19 F+a→n + 22 Na 1274 keV 511keV 3.5-MeV He ++ implantation K-40 Future works Property of Irradiation of DT neutron Property of Irradiation of fast ions Experiment in JT-60 How to insert the CaF2 into ITER Activation method by 19 F( ,n) 22 Na reaction has been started to measure lost  particle


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