Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder

Detalhes bibliográficos
Autor(a) principal: Oliveira, Marcos A. S. de
Data de Publicação: 2011
Outros Autores: Araújo, Cid B. de, Messaddeq, Younes [UNESP]
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UNESP
Texto Completo: http://dx.doi.org/10.1364/OE.19.005620
http://hdl.handle.net/11449/72340
Resumo: An upconversion random laser (RL) operating in the ultraviolet is reported for Nd 3+ doped fluoroindate glass powder pumped at 575 nm. The RL is obtained by the resonant excitation of the Nd 3+ state 2G 7/2 followed by energy transfer among two excited ions such that one ion in the pair decays to a lower energy state and the other is promoted to state 4D 7/2 from where it decays emitting light at 381 nm. The RL threshold of 30 kW/cm 2 was determined by monitoring the photoluminescence intensity as a function of the pump laser intensity. The RL pulses have time duration of 29 ns that is 50 times smaller than the decay time of the upconversion signal when the sample is pumped with intensities below the RL laser threshold. © 2011 Optical Society of America.
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spelling Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powderDecay timeExcited ionsFluoroindate glassLaser thresholdLower energiesPhotoluminescence intensitiesPump laserRandom lasersRandom lasingResonant excitationTime durationUp-conversionEnergy transferGlassNeodymiumOptical pumpingUltraviolet lasersExcited statesAn upconversion random laser (RL) operating in the ultraviolet is reported for Nd 3+ doped fluoroindate glass powder pumped at 575 nm. The RL is obtained by the resonant excitation of the Nd 3+ state 2G 7/2 followed by energy transfer among two excited ions such that one ion in the pair decays to a lower energy state and the other is promoted to state 4D 7/2 from where it decays emitting light at 381 nm. The RL threshold of 30 kW/cm 2 was determined by monitoring the photoluminescence intensity as a function of the pump laser intensity. The RL pulses have time duration of 29 ns that is 50 times smaller than the decay time of the upconversion signal when the sample is pumped with intensities below the RL laser threshold. © 2011 Optical Society of America.Departamento de Física Universidade Federal de Pernambuco, 50670-901 Recife, PEInstituto de Química Universidade do Estado de São Paulo, 14801-970 Araraquara, SPUniversidade Federal de Pernambuco (UFPE)Universidade Estadual Paulista (Unesp)Oliveira, Marcos A. S. deAraújo, Cid B. deMessaddeq, Younes [UNESP]2014-05-27T11:25:30Z2014-05-27T11:25:30Z2011-03-14info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article5620-5626application/pdfhttp://dx.doi.org/10.1364/OE.19.005620Optics Express, v. 19, n. 6, p. 5620-5626, 2011.1094-4087http://hdl.handle.net/11449/7234010.1364/OE.19.0056202-s2.0-799526157422-s2.0-79952615742.pdf2998503841917815Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengOptics Express3.3561,519info:eu-repo/semantics/openAccess2024-01-10T06:27:05Zoai:repositorio.unesp.br:11449/72340Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-01-10T06:27:05Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false
dc.title.none.fl_str_mv Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
title Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
spellingShingle Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
Oliveira, Marcos A. S. de
Decay time
Excited ions
Fluoroindate glass
Laser threshold
Lower energies
Photoluminescence intensities
Pump laser
Random lasers
Random lasing
Resonant excitation
Time duration
Up-conversion
Energy transfer
Glass
Neodymium
Optical pumping
Ultraviolet lasers
Excited states
title_short Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
title_full Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
title_fullStr Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
title_full_unstemmed Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
title_sort Upconversion ultraviolet random lasing in Nd 3+ doped fluoroindate glass powder
author Oliveira, Marcos A. S. de
author_facet Oliveira, Marcos A. S. de
Araújo, Cid B. de
Messaddeq, Younes [UNESP]
author_role author
author2 Araújo, Cid B. de
Messaddeq, Younes [UNESP]
author2_role author
author
dc.contributor.none.fl_str_mv Universidade Federal de Pernambuco (UFPE)
Universidade Estadual Paulista (Unesp)
dc.contributor.author.fl_str_mv Oliveira, Marcos A. S. de
Araújo, Cid B. de
Messaddeq, Younes [UNESP]
dc.subject.por.fl_str_mv Decay time
Excited ions
Fluoroindate glass
Laser threshold
Lower energies
Photoluminescence intensities
Pump laser
Random lasers
Random lasing
Resonant excitation
Time duration
Up-conversion
Energy transfer
Glass
Neodymium
Optical pumping
Ultraviolet lasers
Excited states
topic Decay time
Excited ions
Fluoroindate glass
Laser threshold
Lower energies
Photoluminescence intensities
Pump laser
Random lasers
Random lasing
Resonant excitation
Time duration
Up-conversion
Energy transfer
Glass
Neodymium
Optical pumping
Ultraviolet lasers
Excited states
description An upconversion random laser (RL) operating in the ultraviolet is reported for Nd 3+ doped fluoroindate glass powder pumped at 575 nm. The RL is obtained by the resonant excitation of the Nd 3+ state 2G 7/2 followed by energy transfer among two excited ions such that one ion in the pair decays to a lower energy state and the other is promoted to state 4D 7/2 from where it decays emitting light at 381 nm. The RL threshold of 30 kW/cm 2 was determined by monitoring the photoluminescence intensity as a function of the pump laser intensity. The RL pulses have time duration of 29 ns that is 50 times smaller than the decay time of the upconversion signal when the sample is pumped with intensities below the RL laser threshold. © 2011 Optical Society of America.
publishDate 2011
dc.date.none.fl_str_mv 2011-03-14
2014-05-27T11:25:30Z
2014-05-27T11:25:30Z
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/10.1364/OE.19.005620
Optics Express, v. 19, n. 6, p. 5620-5626, 2011.
1094-4087
http://hdl.handle.net/11449/72340
10.1364/OE.19.005620
2-s2.0-79952615742
2-s2.0-79952615742.pdf
2998503841917815
url http://dx.doi.org/10.1364/OE.19.005620
http://hdl.handle.net/11449/72340
identifier_str_mv Optics Express, v. 19, n. 6, p. 5620-5626, 2011.
1094-4087
10.1364/OE.19.005620
2-s2.0-79952615742
2-s2.0-79952615742.pdf
2998503841917815
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Optics Express
3.356
1,519
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.format.none.fl_str_mv 5620-5626
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
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