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Mechanisms of luminescence decay in YAG-Ce,Mg fibers excited by γ- and X-rays
Time-resolved luminescence of YAG-Ce (150 ppm) fiber crystal with Mg co-doping was studied under pulsed Xray excitation and γ-rays (Cs 662 keV). The initial part of decay kinetics under X-ray excitation is faster than for direct cerium excitation (63 ns). Decay kinetics is also characterized by the...
Autores principales: | , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.optmat.2019.04.054 http://cds.cern.ch/record/2801675 |
Sumario: | Time-resolved luminescence of YAG-Ce (150 ppm) fiber crystal with Mg co-doping was studied under pulsed Xray excitation and γ-rays (Cs 662 keV). The initial part of decay kinetics under X-ray excitation is faster than for
direct cerium excitation (63 ns). Decay kinetics is also characterized by the presence of slow components with at
least two characteristic times longer than Ce$^{3+}$ radiation time. The slowest one which dominates for t > 500 ns
in YAG-Ce without Mg co-doping practically vanishes for samples with 50 ppm co-doping. Decay kinetics under
γ-rays are characterized by slower rise time than that under X-rays. These properties can be explained by
competition of energy transfer and energy losses in track regions. The distribution of excitations in tracks
produced by X-rays differs from that in tracks produced by γ-rays, since the energy of primary electron after γquantum conversion is much higher than after X-ray absorption. The stopping power for energetic electrons
decreases with increase of electron energy, and therefore the density distribution after X-ray conversion is
shifted to higher densities, Therefore, the acceleration of recombination and quenching of excitations is more
prominent under X-ray excitation. Specific role of Ce$^{4+}$ induced by Mg co-doping is also discussed in the paper |
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