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Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor

Novel near-infrared (NIR) phosphors are in demand for light-emitting diode (LED) devices to extend their suitability for new applications and, in turn, support the sustainable and healthy development of the LED industry. The Cr(3+) has been used as an activator in the development of new NIR phosphor...

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Autores principales: Chen, Lei, Wu, Yabing, Liu, Qi, Guo, Yanguang, Liu, Fanghai, Wang, Bo, Wei, Shizhong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9921283/
https://www.ncbi.nlm.nih.gov/pubmed/36770237
http://dx.doi.org/10.3390/ma16031231
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author Chen, Lei
Wu, Yabing
Liu, Qi
Guo, Yanguang
Liu, Fanghai
Wang, Bo
Wei, Shizhong
author_facet Chen, Lei
Wu, Yabing
Liu, Qi
Guo, Yanguang
Liu, Fanghai
Wang, Bo
Wei, Shizhong
author_sort Chen, Lei
collection PubMed
description Novel near-infrared (NIR) phosphors are in demand for light-emitting diode (LED) devices to extend their suitability for new applications and, in turn, support the sustainable and healthy development of the LED industry. The Cr(3+) has been used as an activator in the development of new NIR phosphors. However, one main obstacle for the Cr(3+)-activated phosphors is the low luminescence efficiency due to the spin-forbidden d-d transition of Cr(3+). The rare-earth (RE) huntite minerals that crystallize in the form of REM(3)(BO(3))(4) (M = Al, Sc, Cr, Fe, Ga) have a large family of members, including the rare-earth scandium borates of RESc(3)(BO(3))(4). Interestingly, in our research, we found that the luminescence efficiency of Cr(3+) in the CeSc(3)(BO(3))(4) host, whose quantum yield was measured at 56%, is several times higher than that in GdSc(3)(BO(3))(4), TbSc(3)(BO(3))(4), and LuSc(3)(BO(3))(4) hosts. Hereby, the energy conversion and transfer in the luminescence of CeSc(3)(BO(3))(4):Cr(3+) phosphor were examined. The Stokes shift of electron energy conversion within the Cr(3+ 4)T(2g) level for the emission at 818 nm and excitation at 625 nm in CeSc(3)(BO(3))(4) host was evaluated to be 3775.1 cm(−1), and the super-large splitting energy of the (2)F(5/2) and (2)F(72) sub-states of the Ce(3+) 4f(1) state, about 3000 cm(−1), was found in CeSc(3)(BO(3))(4) host. The typical electronic thermal vibration peaks were observed in the excitation spectra of CeSc(3)(BO(3))(4):Cr(3+). On this basis, the smallest phonon energy, around 347.7 cm(−1), of the CeSc(3)(BO(3))(4) host was estimated. Finally, the energy transfer that is responsible for the far higher photoluminescence of Cr(3+) in CeSc(3)(BO(3))(4) than in other hosts was proven through the way of Ce(3+) emission and Cr(3+) reabsorption.
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spelling pubmed-99212832023-02-12 Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor Chen, Lei Wu, Yabing Liu, Qi Guo, Yanguang Liu, Fanghai Wang, Bo Wei, Shizhong Materials (Basel) Article Novel near-infrared (NIR) phosphors are in demand for light-emitting diode (LED) devices to extend their suitability for new applications and, in turn, support the sustainable and healthy development of the LED industry. The Cr(3+) has been used as an activator in the development of new NIR phosphors. However, one main obstacle for the Cr(3+)-activated phosphors is the low luminescence efficiency due to the spin-forbidden d-d transition of Cr(3+). The rare-earth (RE) huntite minerals that crystallize in the form of REM(3)(BO(3))(4) (M = Al, Sc, Cr, Fe, Ga) have a large family of members, including the rare-earth scandium borates of RESc(3)(BO(3))(4). Interestingly, in our research, we found that the luminescence efficiency of Cr(3+) in the CeSc(3)(BO(3))(4) host, whose quantum yield was measured at 56%, is several times higher than that in GdSc(3)(BO(3))(4), TbSc(3)(BO(3))(4), and LuSc(3)(BO(3))(4) hosts. Hereby, the energy conversion and transfer in the luminescence of CeSc(3)(BO(3))(4):Cr(3+) phosphor were examined. The Stokes shift of electron energy conversion within the Cr(3+ 4)T(2g) level for the emission at 818 nm and excitation at 625 nm in CeSc(3)(BO(3))(4) host was evaluated to be 3775.1 cm(−1), and the super-large splitting energy of the (2)F(5/2) and (2)F(72) sub-states of the Ce(3+) 4f(1) state, about 3000 cm(−1), was found in CeSc(3)(BO(3))(4) host. The typical electronic thermal vibration peaks were observed in the excitation spectra of CeSc(3)(BO(3))(4):Cr(3+). On this basis, the smallest phonon energy, around 347.7 cm(−1), of the CeSc(3)(BO(3))(4) host was estimated. Finally, the energy transfer that is responsible for the far higher photoluminescence of Cr(3+) in CeSc(3)(BO(3))(4) than in other hosts was proven through the way of Ce(3+) emission and Cr(3+) reabsorption. MDPI 2023-01-31 /pmc/articles/PMC9921283/ /pubmed/36770237 http://dx.doi.org/10.3390/ma16031231 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Chen, Lei
Wu, Yabing
Liu, Qi
Guo, Yanguang
Liu, Fanghai
Wang, Bo
Wei, Shizhong
Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title_full Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title_fullStr Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title_full_unstemmed Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title_short Energy Conversion and Transfer in the Luminescence of CeSc(3)(BO(3))(4):Cr(3+) Phosphor
title_sort energy conversion and transfer in the luminescence of cesc(3)(bo(3))(4):cr(3+) phosphor
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9921283/
https://www.ncbi.nlm.nih.gov/pubmed/36770237
http://dx.doi.org/10.3390/ma16031231
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