2016
DOI: 10.1088/1748-0221/11/03/p03013
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Study of radiation hardness of pure CsI crystals for Belle-II calorimeter

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Cited by 9 publications
(4 citation statements)
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References 13 publications
(21 reference statements)
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“…The purpose of this work is to quantify the radiation hardness of 30 cm long CsI(Tl) crystals at uniform doses up to 1000 Gy using spare crystal samples from the Belle and BABAR experiments. With current estimates, in the 10 year lifetime of the Belle II experiment the accumulated dose in crystals in the Belle II endcaps could reach 100 Gy [14]. Our measurement up to 1000 Gy provides an additional factor of 10 safety factor beyond these estimates.…”
Section: Introductionmentioning
confidence: 60%
“…The purpose of this work is to quantify the radiation hardness of 30 cm long CsI(Tl) crystals at uniform doses up to 1000 Gy using spare crystal samples from the Belle and BABAR experiments. With current estimates, in the 10 year lifetime of the Belle II experiment the accumulated dose in crystals in the Belle II endcaps could reach 100 Gy [14]. Our measurement up to 1000 Gy provides an additional factor of 10 safety factor beyond these estimates.…”
Section: Introductionmentioning
confidence: 60%
“…Illustrating this, the recent -1 -report by the KOTO experiment [1] was the first demonstration of energetic neutron vs. photon separation using pulse shape discrimination in pure CsI. The fast timing and radiation hardness of pure CsI [11][12][13] allow it to find application at several recent particle and nuclear physics experiments including KOTO [1], PIENU [14], and PIBETA [15] as well as planned use in the future experiments Mu2e [16] and the Super Charm-Tau Factory [13,17,18]. In this paper the pulse shape discrimination capabilities of pure CsI are explored further by comparing the scintillation response to energy deposits from energetic neutrons and cosmic muons.…”
Section: Introductionmentioning
confidence: 91%
“…The electromagnetic calorimeter (ECAL), as an important part of the spectrometer, in addition to high-efficiency and highprecision gamma detection, also needs good enough time performance for background suppression and gamma-hadron discrimination, etc [2]. Due to the high background level induced by the high luminosity in STCF experiment, pure CsI is selected as the scintillation crystal owing to its fast response, high mass density and good radiation hardness [3,4]. Considering the relatively low light yield of pure CsI crystal, the scintillation light is converted by avalanche photodiode (APD) to obtain an internal gain of 50.…”
Section: Introductionmentioning
confidence: 99%