Confocal and time-resolved photoluminescence spectra of MgAl₂O₄ spinel crystals irradiated with swift heavy bismuth ions

Laser confocal microscopy technique (60 ps laser pulse excitation at 445 nm) and a time-correlated single photon counting (TCSPC) technique have been used to study photoluminescence (PL) in 710 MeV Bi ion irradiated MgAl2O4 single crystals. It was shown that radiation defects produced by swift Bi ions give rise to luminescence with peak at 1.9 eV. Gaussian deconvolution of the PL spectrum reveals that the band consists of three components: the first with a peak at 1.8 eV, the second at 2.1 eV, and the third at 2.35 eV. For the spinel sample irradiated to a fluence of Φ = 1×10¹² ions/cm², both PL and time-resolved photoluminescence (TRPL) spectra were measured as a function of depth within the irradiated layer using a confocal geometry. It was found that with increasing energy loss due to elastic collisions, the PL peak undergoes a redshift, which is more pronounced compared to surface emission measurements.

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Publication Details

Journal
Technobius physics.
Published
2025-06-30
DOI
https://doi.org/10.54355/tbusphys/3.2.2025.0034
Primary Topic
Nuclear materials and radiation effects
Type
article
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article

Confocal and time-resolved photoluminescence spectra of MgAl₂O₄ spinel crystals irradiated with swift heavy bismuth ions

Abdirash T. Akilbekov, N.S. Kirilkin, Meruert Mamatova
Technobius physics.
Nuclear materials and radiation effects
article

Confocal and time-resolved photoluminescence spectra of MgAl₂O₄ spinel crystals irradiated with swift heavy bismuth ions

Abdirash T. Akilbekov, N.S. Kirilkin, Meruert Mamatova
article en

Abstract

Laser confocal microscopy technique (60 ps laser pulse excitation at 445 nm) and a time-correlated single photon counting (TCSPC) technique have been used to study photoluminescence (PL) in 710 MeV Bi ion irradiated MgAl2O4 single crystals. It was shown that radiation defects produced by swift Bi ions give rise to luminescence with peak at 1.9 eV. Gaussian deconvolution of the PL spectrum reveals that the band consists of three components: the first with a peak at 1.8 eV, the second at 2.1 eV, and the third at 2.35 eV. For the spinel sample irradiated to a fluence of Φ = 1×10¹² ions/cm², both PL and time-resolved photoluminescence (TRPL) spectra were measured as a function of depth within the irradiated layer using a confocal geometry. It was found that with increasing energy loss due to elastic collisions, the PL peak undergoes a redshift, which is more pronounced compared to surface emission measurements.

Technobius physics.Vol. 3(2)
L. N. Gumilyov Eurasian National University (KZ), Joint Institute for Nuclear Research (RU)
Affordable and clean energy
Openalex Percentile: Top 85%
Nuclear materials and radiation effects
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