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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container_title | Journal of applied physics |
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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 |
format | Article |
fullrecord | <record><control><sourceid>scitation</sourceid><recordid>TN_cdi_scitation_primary_10_1063_1_3129624Population_inversion</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>jap</sourcerecordid><originalsourceid>FETCH-scitation_primary_10_1063_1_3129624Population_inversion3</originalsourceid><addsrcrecordid>eNqlkM1OwzAMxyMEEmVw4A18Rx1xu49mBy6IjQOaOOyyU5R1GQQl7YhTRJ-GVyUZEzwAF9v62_75g7Fr5EPkk_IWhyUWYlKMTliGvBL5dDzmpyzjvMC8ElNxzi6I3jhHrEqRsa_ndt9ZFUzbgGk-tKcUtTtYAMII9Gdtgt4CBRV0klcOSrg5lFIwLyolNz04rRqK6aZz2ptaWaDWdolKqSu8avCJoN879aNST0G7CIL1BmaJO4PlNpons57HybWPBcpesrOdsqSvjn7A7uYPq_vHnOJiB5Tce-OU7yVymV4gUR5f8Hea_D2t_DfgGx-4cf4</addsrcrecordid><sourcetype>Publisher</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><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><source>AIP Journals Complete</source><source>AIP Digital Archive</source><source>Alma/SFX Local Collection</source><creator>Librantz, André Felipe Henriques ; Gomes, Laércio ; Courrol, Lilia Coronato ; Ranieri, Izilda Marcia ; Baldochi, Sonia Lícia</creator><creatorcontrib>Librantz, André Felipe Henriques ; Gomes, Laércio ; Courrol, Lilia Coronato ; Ranieri, Izilda Marcia ; Baldochi, Sonia Lícia</creatorcontrib><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.</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. On the other hand, a population inversion was not observed for the case of 960 nm
(
Yb
3
+
)
pumping.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqlkM1OwzAMxyMEEmVw4A18Rx1xu49mBy6IjQOaOOyyU5R1GQQl7YhTRJ-GVyUZEzwAF9v62_75g7Fr5EPkk_IWhyUWYlKMTliGvBL5dDzmpyzjvMC8ElNxzi6I3jhHrEqRsa_ndt9ZFUzbgGk-tKcUtTtYAMII9Gdtgt4CBRV0klcOSrg5lFIwLyolNz04rRqK6aZz2ptaWaDWdolKqSu8avCJoN879aNST0G7CIL1BmaJO4PlNpons57HybWPBcpesrOdsqSvjn7A7uYPq_vHnOJiB5Tce-OU7yVymV4gUR5f8Hea_D2t_DfgGx-4cf4</recordid><startdate>20090601</startdate><enddate>20090601</enddate><creator>Librantz, André Felipe Henriques</creator><creator>Gomes, Laércio</creator><creator>Courrol, Lilia Coronato</creator><creator>Ranieri, Izilda Marcia</creator><creator>Baldochi, Sonia Lícia</creator><general>American Institute of Physics</general><scope/></search><sort><creationdate>20090601</creationdate><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><author>Librantz, André Felipe Henriques ; Gomes, Laércio ; Courrol, Lilia Coronato ; Ranieri, Izilda Marcia ; Baldochi, Sonia Lícia</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-scitation_primary_10_1063_1_3129624Population_inversion3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><creationdate>2009</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><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><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Librantz, André Felipe Henriques</au><au>Gomes, Laércio</au><au>Courrol, Lilia Coronato</au><au>Ranieri, Izilda Marcia</au><au>Baldochi, Sonia Lícia</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>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</atitle><jtitle>Journal of applied physics</jtitle><date>2009-06-01</date><risdate>2009</risdate><volume>105</volume><issue>11</issue><spage>113503</spage><epage>113503-10</epage><pages>113503-113503-10</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>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.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.3129624</doi></addata></record> |
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source | AIP Journals Complete; AIP Digital Archive; Alma/SFX Local Collection |
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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