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Highly Luminous N(3–)-Substituted Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting Diodes
[Image: see text] The N(3–)-substituted Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors were systematically prepared and analyzed. Secondary-ion mass spectroscopy measurements revealed that the average N(3–) contents are 0.003 for Ca, 0.009 for Sr, and 0.032 for Ba. Furthermore, the N(3–) incorpo...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2019
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6648572/ https://www.ncbi.nlm.nih.gov/pubmed/31459932 http://dx.doi.org/10.1021/acsomega.8b03489 |
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author | Kim, Donghyeon Ji, Choon Woo Lee, Jungjun Bae, Jong-Seong Hong, Tae Eun Ahn, Sung Il Chung, In Kim, Seung-Joo Park, Jung-Chul |
author_facet | Kim, Donghyeon Ji, Choon Woo Lee, Jungjun Bae, Jong-Seong Hong, Tae Eun Ahn, Sung Il Chung, In Kim, Seung-Joo Park, Jung-Chul |
author_sort | Kim, Donghyeon |
collection | PubMed |
description | [Image: see text] The N(3–)-substituted Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors were systematically prepared and analyzed. Secondary-ion mass spectroscopy measurements revealed that the average N(3–) contents are 0.003 for Ca, 0.009 for Sr, and 0.032 for Ba. Furthermore, the N(3–) incorporation in the host lattices was corroborated by infrared and X-ray photoelectron spectroscopies. From the photoluminescence spectra of Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors before and after N(3–) doping, it was verified that the enhanced emission intensity of the phosphors is most likely due to the N(3–) doping. In Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors, the maximum wavelengths of the emission band were red-shifted in the order Ca < Ba < Sr, which is not consistent with the trend of crystal field splitting: Ba < Sr < Ca. This discrepancy was clearly explained by electron–electron repulsions among polyhedra, LiO(4)–MO(n), SiO(4)–MO(n), and MO(n)–M’O(n) associated with structural difference in the host lattices. Therefore, the energy levels associated with the 4f(6)5d energy levels of Eu(2+) are definitely established in the following order: Li(2)CaSiO(4):Eu(2+) > Li(2)BaSiO(4):Eu(2+) > Li(2)SrSiO(4):Eu(2+). Furthermore, using the Williamson–Hall (W–H) method, the determined structural strains of Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors revealed that the increased compressive strain after N(3–) doping induces the enhanced emission intensity of these phosphors. White light-emitting diodes made by three N(3–)-doped phosphors and a 365 nm emitting InGaN chip showed the (0.333, 0.373) color coordinate and high color-rendering index (R(a) = 83). These phosphor materials may provide a platform for development of new efficient phosphors in solid-state lighting field. |
format | Online Article Text |
id | pubmed-6648572 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-66485722019-08-27 Highly Luminous N(3–)-Substituted Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting Diodes Kim, Donghyeon Ji, Choon Woo Lee, Jungjun Bae, Jong-Seong Hong, Tae Eun Ahn, Sung Il Chung, In Kim, Seung-Joo Park, Jung-Chul ACS Omega [Image: see text] The N(3–)-substituted Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors were systematically prepared and analyzed. Secondary-ion mass spectroscopy measurements revealed that the average N(3–) contents are 0.003 for Ca, 0.009 for Sr, and 0.032 for Ba. Furthermore, the N(3–) incorporation in the host lattices was corroborated by infrared and X-ray photoelectron spectroscopies. From the photoluminescence spectra of Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors before and after N(3–) doping, it was verified that the enhanced emission intensity of the phosphors is most likely due to the N(3–) doping. In Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors, the maximum wavelengths of the emission band were red-shifted in the order Ca < Ba < Sr, which is not consistent with the trend of crystal field splitting: Ba < Sr < Ca. This discrepancy was clearly explained by electron–electron repulsions among polyhedra, LiO(4)–MO(n), SiO(4)–MO(n), and MO(n)–M’O(n) associated with structural difference in the host lattices. Therefore, the energy levels associated with the 4f(6)5d energy levels of Eu(2+) are definitely established in the following order: Li(2)CaSiO(4):Eu(2+) > Li(2)BaSiO(4):Eu(2+) > Li(2)SrSiO(4):Eu(2+). Furthermore, using the Williamson–Hall (W–H) method, the determined structural strains of Li(2)MSiO(4):Eu(2+) (M = Ca, Sr, and Ba) phosphors revealed that the increased compressive strain after N(3–) doping induces the enhanced emission intensity of these phosphors. White light-emitting diodes made by three N(3–)-doped phosphors and a 365 nm emitting InGaN chip showed the (0.333, 0.373) color coordinate and high color-rendering index (R(a) = 83). These phosphor materials may provide a platform for development of new efficient phosphors in solid-state lighting field. American Chemical Society 2019-05-13 /pmc/articles/PMC6648572/ /pubmed/31459932 http://dx.doi.org/10.1021/acsomega.8b03489 Text en Copyright © 2019 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Kim, Donghyeon Ji, Choon Woo Lee, Jungjun Bae, Jong-Seong Hong, Tae Eun Ahn, Sung Il Chung, In Kim, Seung-Joo Park, Jung-Chul Highly Luminous N(3–)-Substituted Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting Diodes |
title | Highly Luminous N(3–)-Substituted
Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting
Diodes |
title_full | Highly Luminous N(3–)-Substituted
Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting
Diodes |
title_fullStr | Highly Luminous N(3–)-Substituted
Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting
Diodes |
title_full_unstemmed | Highly Luminous N(3–)-Substituted
Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting
Diodes |
title_short | Highly Luminous N(3–)-Substituted
Li(2)MSiO(4−δ)N(2/3δ):Eu(2+) (M = Ca, Sr, and Ba) for White NUV Light-Emitting
Diodes |
title_sort | highly luminous n(3–)-substituted
li(2)msio(4−δ)n(2/3δ):eu(2+) (m = ca, sr, and ba) for white nuv light-emitting
diodes |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6648572/ https://www.ncbi.nlm.nih.gov/pubmed/31459932 http://dx.doi.org/10.1021/acsomega.8b03489 |
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