Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses
Autor(a) principal: | |
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Data de Publicação: | 1996 |
Outros Autores: | , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UNESP |
Texto Completo: | http://dx.doi.org/10.1103/PhysRevB.53.6065 http://hdl.handle.net/11449/64746 |
Resumo: | Fluorindate glasses containing 1,2,3,4 ErF3 mol % were prepared in a dry box under argon atmosphere. Absorption, Stokes luminescence (under visible and infrared excitation), the dependence of 4S3/2, 4I11/2, and 4I13/2 lifetimes with Er concentration, and upconversion under Ti-saphire laser excitation at λ=790 nm were measured, mostly at T=77 and 300 K. The upconversion results in a strong green emission and weaker blue and red emissions whose intensity obeys a power-law behavior I∼Pn, where P is the infrared excitation power and n=1.6, 2.1, and 2.9 for the red, green, and blue emissions, respectively. The red emission exponent n=1.5 can be explained by a cross relaxation process. The green and blue emissions are due to excited state absorption (ESA) and energy transfer (ET) processes that predict a factor n=2 and n=3 for the green and blue emissions, respectively. From transient measurements we concluded that for lightly doped samples the green upconverted emission is originated due to both processes ESA and ET. However, for heavily doped samples ET is the dominant process. |
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Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glassesFluorindate glasses containing 1,2,3,4 ErF3 mol % were prepared in a dry box under argon atmosphere. Absorption, Stokes luminescence (under visible and infrared excitation), the dependence of 4S3/2, 4I11/2, and 4I13/2 lifetimes with Er concentration, and upconversion under Ti-saphire laser excitation at λ=790 nm were measured, mostly at T=77 and 300 K. The upconversion results in a strong green emission and weaker blue and red emissions whose intensity obeys a power-law behavior I∼Pn, where P is the infrared excitation power and n=1.6, 2.1, and 2.9 for the red, green, and blue emissions, respectively. The red emission exponent n=1.5 can be explained by a cross relaxation process. The green and blue emissions are due to excited state absorption (ESA) and energy transfer (ET) processes that predict a factor n=2 and n=3 for the green and blue emissions, respectively. From transient measurements we concluded that for lightly doped samples the green upconverted emission is originated due to both processes ESA and ET. However, for heavily doped samples ET is the dominant process.Inst. de Fis. de São Carlos Universidade de Sâo Paulo, Caixa Postal 369, 13560-970 São Carlos, SPInstituto de Química Univ. Estadual de São Paulo, Araraquara, São PauloInst. de Fis. de São Carlos Universidade de São Paulo, Caixa Postal 369, 13560-970 São Carlos, SPUniversidade Estadual Paulista (Unesp)Universidade de São Paulo (USP)Catunda, T.Nunes, L. A. O.Florez, A.Messaddeq, Younes [UNESP]Aegerter, M. A.2014-05-27T11:18:04Z2014-05-27T11:18:04Z1996-03-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article6065-6070application/pdfhttp://dx.doi.org/10.1103/PhysRevB.53.6065Physical Review B - Condensed Matter and Materials Physics, v. 53, n. 10, p. 6065-6070, 1996.0163-1829http://hdl.handle.net/11449/6474610.1103/PhysRevB.53.60652-s2.0-00009818072-s2.0-0000981807.pdf2998503841917815Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengPhysical Review B: Condensed Matter and Materials Physics1,176info:eu-repo/semantics/openAccess2023-11-08T06:10:57Zoai:repositorio.unesp.br:11449/64746Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T17:09:43.612359Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false |
dc.title.none.fl_str_mv |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
title |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
spellingShingle |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses Catunda, T. |
title_short |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
title_full |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
title_fullStr |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
title_full_unstemmed |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
title_sort |
Spectroscopic properties and upconversion mechanisms in Er3+-doped fluoroindate glasses |
author |
Catunda, T. |
author_facet |
Catunda, T. Nunes, L. A. O. Florez, A. Messaddeq, Younes [UNESP] Aegerter, M. A. |
author_role |
author |
author2 |
Nunes, L. A. O. Florez, A. Messaddeq, Younes [UNESP] Aegerter, M. A. |
author2_role |
author author author author |
dc.contributor.none.fl_str_mv |
Universidade Estadual Paulista (Unesp) Universidade de São Paulo (USP) |
dc.contributor.author.fl_str_mv |
Catunda, T. Nunes, L. A. O. Florez, A. Messaddeq, Younes [UNESP] Aegerter, M. A. |
description |
Fluorindate glasses containing 1,2,3,4 ErF3 mol % were prepared in a dry box under argon atmosphere. Absorption, Stokes luminescence (under visible and infrared excitation), the dependence of 4S3/2, 4I11/2, and 4I13/2 lifetimes with Er concentration, and upconversion under Ti-saphire laser excitation at λ=790 nm were measured, mostly at T=77 and 300 K. The upconversion results in a strong green emission and weaker blue and red emissions whose intensity obeys a power-law behavior I∼Pn, where P is the infrared excitation power and n=1.6, 2.1, and 2.9 for the red, green, and blue emissions, respectively. The red emission exponent n=1.5 can be explained by a cross relaxation process. The green and blue emissions are due to excited state absorption (ESA) and energy transfer (ET) processes that predict a factor n=2 and n=3 for the green and blue emissions, respectively. From transient measurements we concluded that for lightly doped samples the green upconverted emission is originated due to both processes ESA and ET. However, for heavily doped samples ET is the dominant process. |
publishDate |
1996 |
dc.date.none.fl_str_mv |
1996-03-01 2014-05-27T11:18:04Z 2014-05-27T11:18:04Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://dx.doi.org/10.1103/PhysRevB.53.6065 Physical Review B - Condensed Matter and Materials Physics, v. 53, n. 10, p. 6065-6070, 1996. 0163-1829 http://hdl.handle.net/11449/64746 10.1103/PhysRevB.53.6065 2-s2.0-0000981807 2-s2.0-0000981807.pdf 2998503841917815 |
url |
http://dx.doi.org/10.1103/PhysRevB.53.6065 http://hdl.handle.net/11449/64746 |
identifier_str_mv |
Physical Review B - Condensed Matter and Materials Physics, v. 53, n. 10, p. 6065-6070, 1996. 0163-1829 10.1103/PhysRevB.53.6065 2-s2.0-0000981807 2-s2.0-0000981807.pdf 2998503841917815 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
Physical Review B: Condensed Matter and Materials Physics 1,176 |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
6065-6070 application/pdf |
dc.source.none.fl_str_mv |
Scopus reponame:Repositório Institucional da UNESP instname:Universidade Estadual Paulista (UNESP) instacron:UNESP |
instname_str |
Universidade Estadual Paulista (UNESP) |
instacron_str |
UNESP |
institution |
UNESP |
reponame_str |
Repositório Institucional da UNESP |
collection |
Repositório Institucional da UNESP |
repository.name.fl_str_mv |
Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP) |
repository.mail.fl_str_mv |
|
_version_ |
1808128763945287680 |