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Scandium and aluminum substitution and energy transfer processes in the undoped and Ce-doped scintillation crystals
Phys. Rev. Materials 10, 045201 – Published 17 April, 2026
DOI: https://doi.org/10.1103/png3-xnt7
Abstract
The structural and scintillation properties of pure and Ce-doped crystals were systematically investigated. High-resolution and magic angle spinning nuclear magnetic resonance spectroscopy revealed that ions predominantly occupy octahedral sites, effectively replacing ions, while antisite Sc at Y dodecahedral positions remains below 0.2 at.%. Sc incorporation into induces strong exciton emission at 320–324 nm, nearly 10 times higher than that of reference (BGO) crystal, even at low Sc concentrations (5 at.%). doping introduces characteristic emission at 518 nm, accelerates scintillation decay, and in combination with codoping, promotes the formation of ions that enable a fast radiative de-excitation pathway. : Ce exhibits a maximum scintillation light yield of 80–84% relative to BGO with a mean decay time of 85–110 ns. Thermostimulated liminescence and electron paramagnetic resonance studies indicate that holes are mainly trapped at oxygen ions near Sc ions ( centers), while electrons are primarily localized at Sc antisite ions near oxygen vacancies ( centers), affecting scintillation kinetics. Density functional theory calculations confirm that at the dodecahedral site forms a deep electron trap. These results highlight the key role of Sc and Ce in tuning emission, decay dynamics, and defect-mediated processes in Sc-admixed multicomponent garnet scintillators.
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References (59)
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