Population inversion of G 1 4 excited state of Tm 3 + investigated by meansof numerical solutions of the rate equations system in Yb : Tm : Nd : LiYF 4 crystal

In this work we present the spectroscopic properties of LiYF 4 (YLF) single crystals activated with thulium and codoped with ytterbium and neodymium ions. The most important processes that lead to the thulium upconversion emissions in the blue region were identified. A time-resolved luminescence spe...

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Veröffentlicht in:Journal of applied physics 2009-06, Vol.105 (11), p.113503-113503-10
Hauptverfasser: Librantz, André Felipe Henriques, Gomes, Laércio, Courrol, Lilia Coronato, Ranieri, Izilda Marcia, Baldochi, Sonia Lícia
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container_end_page 113503-10
container_issue 11
container_start_page 113503
container_title Journal of applied physics
container_volume 105
creator Librantz, André Felipe Henriques
Gomes, Laércio
Courrol, Lilia Coronato
Ranieri, Izilda Marcia
Baldochi, Sonia Lícia
description In this work we present the spectroscopic properties of LiYF 4 (YLF) single crystals activated with thulium and codoped with ytterbium and neodymium ions. The most important processes that lead to the thulium upconversion emissions in the blue region were identified. A time-resolved luminescence spectroscopy technique was employed to measure the luminescence decays and to determine the most important mechanisms involved in the upconversion process that populates G 1 4 ( Tm 3 + ) excited state. Analysis of the energy transfer processes dynamics using selective pulsed laser excitations in Yb:Tm:Nd, Tm:Nd, and Tm:Yb YLF crystals shows that the energy transfer from Nd 3 + to Yb 3 + ions is the mechanism responsible for the enhancement in the blue upconversion efficiency in the Yb:Tm:Nd:YLF when compared with the Yb:Tm system. A study of the energy transfer processes in YLF:Yb:Tm:Nd crystal showed that the G 1 4 excited level is mainly populated by a sequence of two nonradiative energy transfers that start well after the Nd 3 + and Tm 3 + excitations at 797 nm according to Nd 3 + ( F 4 3 / 2 ) → Yb 3 + ( F 2 7 / 2 ) , followed by Yb 3 + ( F 2 5 / 2 ) → Tm ( H 3 4 ) → Tm 3 + ( G 1 4 ) . Results of numerical simulation of the rate equations system showed that a population inversion for 481.4 nm laser emission line is attained for a pumping rate threshold of 26   s − 1 , which is equivalent to an intensity of 880   W cm − 2 for a continuous laser pumping at 797 nm. On the other hand, a population inversion was not observed for the case of 960 nm ( Yb 3 + ) pumping.
doi_str_mv 10.1063/1.3129624
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The most important processes that lead to the thulium upconversion emissions in the blue region were identified. A time-resolved luminescence spectroscopy technique was employed to measure the luminescence decays and to determine the most important mechanisms involved in the upconversion process that populates G 1 4 ( Tm 3 + ) excited state. Analysis of the energy transfer processes dynamics using selective pulsed laser excitations in Yb:Tm:Nd, Tm:Nd, and Tm:Yb YLF crystals shows that the energy transfer from Nd 3 + to Yb 3 + ions is the mechanism responsible for the enhancement in the blue upconversion efficiency in the Yb:Tm:Nd:YLF when compared with the Yb:Tm system. A study of the energy transfer processes in YLF:Yb:Tm:Nd crystal showed that the G 1 4 excited level is mainly populated by a sequence of two nonradiative energy transfers that start well after the Nd 3 + and Tm 3 + excitations at 797 nm according to Nd 3 + ( F 4 3 / 2 ) → Yb 3 + ( F 2 7 / 2 ) , followed by Yb 3 + ( F 2 5 / 2 ) → Tm ( H 3 4 ) → Tm 3 + ( G 1 4 ) . Results of numerical simulation of the rate equations system showed that a population inversion for 481.4 nm laser emission line is attained for a pumping rate threshold of 26   s − 1 , which is equivalent to an intensity of 880   W cm − 2 for a continuous laser pumping at 797 nm. On the other hand, a population inversion was not observed for the case of 960 nm ( Yb 3 + ) pumping.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.3129624</identifier><identifier>CODEN: JAPIAU</identifier><publisher>American Institute of Physics</publisher><ispartof>Journal of applied physics, 2009-06, Vol.105 (11), p.113503-113503-10</ispartof><rights>2009 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-scitation_primary_10_1063_1_3129624Population_inversion3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.3129624$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1559,4512,27924,27925,76384,76390</link.rule.ids></links><search><creatorcontrib>Librantz, André Felipe Henriques</creatorcontrib><creatorcontrib>Gomes, Laércio</creatorcontrib><creatorcontrib>Courrol, Lilia Coronato</creatorcontrib><creatorcontrib>Ranieri, Izilda Marcia</creatorcontrib><creatorcontrib>Baldochi, Sonia Lícia</creatorcontrib><title>Population inversion of G 1 4 excited state of Tm 3 + investigated by meansof numerical solutions of the rate equations system in Yb : Tm : Nd : LiYF 4 crystal</title><title>Journal of applied physics</title><description>In this work we present the spectroscopic properties of LiYF 4 (YLF) single crystals activated with thulium and codoped with ytterbium and neodymium ions. The most important processes that lead to the thulium upconversion emissions in the blue region were identified. A time-resolved luminescence spectroscopy technique was employed to measure the luminescence decays and to determine the most important mechanisms involved in the upconversion process that populates G 1 4 ( Tm 3 + ) excited state. Analysis of the energy transfer processes dynamics using selective pulsed laser excitations in Yb:Tm:Nd, Tm:Nd, and Tm:Yb YLF crystals shows that the energy transfer from Nd 3 + to Yb 3 + ions is the mechanism responsible for the enhancement in the blue upconversion efficiency in the Yb:Tm:Nd:YLF when compared with the Yb:Tm system. A study of the energy transfer processes in YLF:Yb:Tm:Nd crystal showed that the G 1 4 excited level is mainly populated by a sequence of two nonradiative energy transfers that start well after the Nd 3 + and Tm 3 + excitations at 797 nm according to Nd 3 + ( F 4 3 / 2 ) → Yb 3 + ( F 2 7 / 2 ) , followed by Yb 3 + ( F 2 5 / 2 ) → Tm ( H 3 4 ) → Tm 3 + ( G 1 4 ) . Results of numerical simulation of the rate equations system showed that a population inversion for 481.4 nm laser emission line is attained for a pumping rate threshold of 26   s − 1 , which is equivalent to an intensity of 880   W cm − 2 for a continuous laser pumping at 797 nm. 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The most important processes that lead to the thulium upconversion emissions in the blue region were identified. A time-resolved luminescence spectroscopy technique was employed to measure the luminescence decays and to determine the most important mechanisms involved in the upconversion process that populates G 1 4 ( Tm 3 + ) excited state. Analysis of the energy transfer processes dynamics using selective pulsed laser excitations in Yb:Tm:Nd, Tm:Nd, and Tm:Yb YLF crystals shows that the energy transfer from Nd 3 + to Yb 3 + ions is the mechanism responsible for the enhancement in the blue upconversion efficiency in the Yb:Tm:Nd:YLF when compared with the Yb:Tm system. A study of the energy transfer processes in YLF:Yb:Tm:Nd crystal showed that the G 1 4 excited level is mainly populated by a sequence of two nonradiative energy transfers that start well after the Nd 3 + and Tm 3 + excitations at 797 nm according to Nd 3 + ( F 4 3 / 2 ) → Yb 3 + ( F 2 7 / 2 ) , followed by Yb 3 + ( F 2 5 / 2 ) → Tm ( H 3 4 ) → Tm 3 + ( G 1 4 ) . Results of numerical simulation of the rate equations system showed that a population inversion for 481.4 nm laser emission line is attained for a pumping rate threshold of 26   s − 1 , which is equivalent to an intensity of 880   W cm − 2 for a continuous laser pumping at 797 nm. On the other hand, a population inversion was not observed for the case of 960 nm ( Yb 3 + ) pumping.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.3129624</doi></addata></record>
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title Population inversion of G 1 4 excited state of Tm 3 + investigated by meansof numerical solutions of the rate equations system in Yb : Tm : Nd : LiYF 4 crystal
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