2021
DOI: 10.3390/photonics8030071
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A Review on X-ray Excited Emission Decay Dynamics in Inorganic Scintillator Materials

Abstract: Scintillator materials convert high-energy radiation into photons in the ultraviolet to visible light region for radiation detection. In this review, advances in X-ray emission dynamics of inorganic scintillators are presented, including inorganic halides (alkali-metal halides, alkaline-earth halides, rare-earth halides, oxy-halides, rare-earth oxyorthosilicates, halide perovskites), oxides (binary oxides, complex oxides, post-transition metal oxides), sulfides, rare-earth doped scintillators, and organic-inor… Show more

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Cited by 51 publications
(27 citation statements)
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References 172 publications
(198 reference statements)
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“…In terms of luminescent properties, different from conventional direct-bandgap semiconductors represented by zinc oxide (ZnO), gallium nitride (GaN), and aluminum nitride (AlN), the luminescence spectrum of β-Ga 2 O 3 does not show near-band emission (NBE) but strong broad luminescence characteristics composed of several emission components instead in the spectral range of 2.3–4.5 eV. , The lack of NBE is generally attributed to the formation of a self-trapped hole (STH), which is recombined with weakly localized electrons to contribute to a so-called self-trapped exciton emission (STE) in β-Ga 2 O 3 . By studying the STE luminescence of β-Ga 2 O 3 , we can obtain useful physical parameters and information like the strength of electron–phonon coupling and exciton binding energy. Up to now, a detailed temperature-dependent study of the broad-spectrum STE luminescence of β-Ga 2 O 3 is still worth conducting, for which an in-depth study can help deepen the understanding of this STE luminescence mechanism.…”
mentioning
confidence: 76%
“…In terms of luminescent properties, different from conventional direct-bandgap semiconductors represented by zinc oxide (ZnO), gallium nitride (GaN), and aluminum nitride (AlN), the luminescence spectrum of β-Ga 2 O 3 does not show near-band emission (NBE) but strong broad luminescence characteristics composed of several emission components instead in the spectral range of 2.3–4.5 eV. , The lack of NBE is generally attributed to the formation of a self-trapped hole (STH), which is recombined with weakly localized electrons to contribute to a so-called self-trapped exciton emission (STE) in β-Ga 2 O 3 . By studying the STE luminescence of β-Ga 2 O 3 , we can obtain useful physical parameters and information like the strength of electron–phonon coupling and exciton binding energy. Up to now, a detailed temperature-dependent study of the broad-spectrum STE luminescence of β-Ga 2 O 3 is still worth conducting, for which an in-depth study can help deepen the understanding of this STE luminescence mechanism.…”
mentioning
confidence: 76%
“…The excitation spectrum of Ce 3+ emission at 530 nm is composed of three sets of broad bands, which belong to the characteristic excitation transition of Ce 3+ and Tb 3+ ions, respectively. The band peaking at around 340 nm and 450 nm were commonly ascribed to 4f–5d 2 and 4f–5d 1 transition of the Ce 3+ , respectively [ 37 , 38 ]. The sharp lines observed at 302–313 nm are related to the characterized 8S 7/2 –6I j , 6P j excitation transition of Gd 3+ ion [ 39 ].…”
Section: Resultsmentioning
confidence: 99%
“…1029 Rare-earth halides, oxides, oxyhalides, oxysulfides, oxyorthosilicates, and perovskites possess excellent scintillation performance. 1030 In particular, Y, La, Gd, and Lu have been extensively studied as host lattices for controlling radioluminescence. 1031 Rare-earthdoped nanoscintillators with fast decay or persistent luminescence are being developed for specific applications.…”
Section: Photodetectorsmentioning
confidence: 99%