TY - JOUR
T1 - Scintillation and photoluminescence properties of (Tl1−xAx)MgCl3 (where A = alkali metal)
AU - Arai, Miki
AU - Fujimoto, Yutaka
AU - Koshimizu, Masanori
AU - Yanagida, Takayuki
AU - Asai, Keisuke
N1 - Funding Information:
This research was supported by a Grant-in-Aid for Scientific Research (A) (No. 18H03890 , 2018–2021). A part of this research is based on the Cooperative Research Project of Research Center for Biomedical Engineering, Ministry of Education, Culture, Sports, Science and Technology.
Publisher Copyright:
© 2020 Elsevier B.V.
PY - 2020/5/15
Y1 - 2020/5/15
N2 - We developed (Tl1−x Ax)MgCl3 (A = Li, Na, K, Rb, and Cs) crystalline scintillators to improve by cation substitution the scintillation properties of TlMgCl3, for which we have previously reported good scintillation properties (light yield = 46,000 photons/MeV and scintillation decay time constants = 60 ns (∼25%) and 350 ns (∼75%)). The X-ray-induced scintillation spectra of these (Tl1−x Ax)MgCl3 scintillators exhibited an intense emission band at 420 nm, which corresponds to the wavelength observed for TlMgCl3. This means that the light-emitting mechanisms of (Tl1−xAx)MgCl3 are similar to that in TlMgCl3. The light yields of (Tl0.995K0.005)MgCl3 (55,000 photons/MeV) and (Tl0.995Cs0.005)MgCl3 (49,000 photons/MeV) were higher than that of TlMgCl3 (46,000 photons/MeV). This is attributed to the increased number of electron–hole pairs contributing to the scintillation owing to the decreased number of trapped electrons and holes, as revealed by the lower intensity of thermoluminescence. As a result, we succeeded in increasing the light yields by cation substitution.
AB - We developed (Tl1−x Ax)MgCl3 (A = Li, Na, K, Rb, and Cs) crystalline scintillators to improve by cation substitution the scintillation properties of TlMgCl3, for which we have previously reported good scintillation properties (light yield = 46,000 photons/MeV and scintillation decay time constants = 60 ns (∼25%) and 350 ns (∼75%)). The X-ray-induced scintillation spectra of these (Tl1−x Ax)MgCl3 scintillators exhibited an intense emission band at 420 nm, which corresponds to the wavelength observed for TlMgCl3. This means that the light-emitting mechanisms of (Tl1−xAx)MgCl3 are similar to that in TlMgCl3. The light yields of (Tl0.995K0.005)MgCl3 (55,000 photons/MeV) and (Tl0.995Cs0.005)MgCl3 (49,000 photons/MeV) were higher than that of TlMgCl3 (46,000 photons/MeV). This is attributed to the increased number of electron–hole pairs contributing to the scintillation owing to the decreased number of trapped electrons and holes, as revealed by the lower intensity of thermoluminescence. As a result, we succeeded in increasing the light yields by cation substitution.
KW - Radioluminescence
KW - Scintillator
KW - TlMgCl3
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U2 - 10.1016/j.jallcom.2020.153871
DO - 10.1016/j.jallcom.2020.153871
M3 - Article
AN - SCOPUS:85078163408
SN - 0925-8388
VL - 823
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
M1 - 153871
ER -