Bulletin of the American Physical Society
5th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Volume 63, Number 12
Tuesday–Saturday, October 23–27, 2018; Waikoloa, Hawaii
Session MH: Instrumentation V
2:00 PM–4:45 PM,
Saturday, October 27, 2018
Hilton
Room: Kona 2/3
Chair: Shaofei Zhu, Argonne National Laboratory
Abstract ID: BAPS.2018.HAW.MH.2
Abstract: MH.00002 : Development of a gamma-ray tracking detector and its performance test
2:15 PM–2:30 PM
Presenter:
Asahi Kohda
(RCNP, Osaka Univ.)
Authors:
Asahi Kohda
(RCNP, Osaka Univ.)
Nori Aoi
(RCNP, Osaka Univ.)
Yasutaka Yamamoto
(RCNP, Osaka Univ.)
Eiji Ideguchi
(RCNP, Osaka Univ.)
Mukhi Kumar Raju
(RCNP, Osaka Univ.)
Hoang Thi Ha
(RCNP, Osaka Univ.)
Tung Thanh Pham
(RCNP, Osaka Univ.)
Tatsushi Shima
(RCNP, Osaka Univ.)
Viljamaa Topi Benjamin
(Univ. of Jyväskylä, Finland)
Shuji Miyamoto
(Univ. of Hyogo)
Toshiyuki Shizuma
(QST)
Nobuaki Imai
(CNS, Univ. of Tokyo)
Kathrin Wimmer
(Univ. of Tokyo)
Pieter Doornenbal
(RIKEN Nishina Center)
Rudrajyoti Palit
(TIFR, India)
The gamma-ray tracking detector is a germanium detector realizing both high efficiency and Compton background suppression by reconstructing the scattering process of the incident gamma-rays from the positions and energy deposits of the gamma-rays at each interaction points in the detector. Its high position resolution is also beneficial for accurate Doppler correction. In the tracking detector, the interaction positions are determined three-dimensionally with high position resolution by analyzing the signal waveform from the segmented electrodes. We have measured waveforms for different interaction points of gamma-rays using a GRETINA Quad Detector. The experiment was performed using a gamma-ray beam from the GACKO beam line at the NewSUBARU electron storage ring facility. The three dimensional position of the interaction in points are selected first by collimating the incident gamma-rays and then by measuring the gamma-rays scatted at 90 degree in the detector by using a narrow slit. Obtained waveforms were compared with the simulated waveform.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.HAW.MH.2
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