2019
DOI: 10.1016/j.nima.2019.03.065
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Non-linearity effects on the light-output calibration of light charged particles in CsI(Tl) scintillator crystals

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Cited by 31 publications
(20 citation statements)
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References 29 publications
(71 reference statements)
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“…5, the energy response for Z = 1 isotopes exhibits insignificant non-linearity and slight difference among the isotopes in the energy range of 0 − 100 MeV in accordance with the results in Ref. [19]. For the heavy isotopes from He to Boron, however, the non-linearity is increasingly pronounced depending on the species.…”
Section: Energy Calibration Of the Csi(tl) Crystalssupporting
confidence: 90%
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“…5, the energy response for Z = 1 isotopes exhibits insignificant non-linearity and slight difference among the isotopes in the energy range of 0 − 100 MeV in accordance with the results in Ref. [19]. For the heavy isotopes from He to Boron, however, the non-linearity is increasingly pronounced depending on the species.…”
Section: Energy Calibration Of the Csi(tl) Crystalssupporting
confidence: 90%
“…6. The trends of the fitting curves are consistent with the results of HiRA10 detectors [19], and a detailed discussion on the energy calibration of CsI(Tl) crystals can be found therein.…”
Section: Energy Calibration Of the Csi(tl) Crystalssupporting
confidence: 84%
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“…Two types of wedge-shaped CsI(Tl)s were designed to be placed behind the annular double-sided silicon detectors (ADSSDs) to identify the light charged particles with the Δ − method. The properties of CsI(Tl)s with different shapes and sizes, such as energy resolution, light output nonuniformity and particle identification capability, were compared by using a -source and a radioactive beam of 15 C. The big-size CsI(Tl) was finally adopted to form the Δ − telescope due to better properties. The property differences of these two types of CsI(Tl)s can be interpreted based on the Geant4 simulation results.…”
Section: Introductionmentioning
confidence: 99%
“…[8,9,10,11], which decreases the energy resolution of crystals and further affects the particle-identification (PID) capability of the Δ − method. In this paper, we designed two types of wedgeshaped CsI(Tl)s to match the ADSSD size, then tested and compared their energy resolution, PID capability, and light output non-uniformity by using a -source and a radioactive beam of 15 C. Finally, we chose one shape with better properties as the detector of the telescope TA.…”
Section: Introductionmentioning
confidence: 99%