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Low‐dimensional halide perovskites with highly efficient luminescent properties have attracted huge attention in optoelectronic and radiation detection applications in recent years. Herein, a highly efficient 0D Cs 3 Cu 2 I 5 perovskite crystal is presented for X‐ray and γ‐ray detection that can be easily grown from the melt by the Bridgman method. The crystal structure of Cs 3 Cu 2 I 5 belongs to an orthorhombic system with a space group of Pnma . The Cs 3 Cu 2 I 5 crystal is nonhygroscopic and self‐absorption free due to a large Stokes shift of 120 nm originated from its self‐trapped exciton emission. Its scintillation emission centers at 440 nm with a principal decay time of 967 ns. The Cs 3 Cu 2 I 5 crystal not only demonstrates a high scintillation yield of about 32 000 photons MeV −1 and an extremely low afterglow of 0.03% at 10 ms under X‐ray radiation, but also possesses a high light yield of 29 000 photons MeV −1 with an excellent energy resolution of 3.4% at 662 keV under γ‐ray radiation.
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Cheng et al. (2020) studied this question.
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