Spectroscopic properties of the 1.8 μm emission of Tm3+/Yb3+ codoped TeO2-ZnO-Bi2O3 glasses with efficient energy transfer
Identifieur interne : 000233 ( Pascal/Curation ); précédent : 000232; suivant : 000234Spectroscopic properties of the 1.8 μm emission of Tm3+/Yb3+ codoped TeO2-ZnO-Bi2O3 glasses with efficient energy transfer
Auteurs : KEFENG LI [République populaire de Chine] ; SIJUN FAN [République populaire de Chine] ; LEI ZHANG [République populaire de Chine] ; QIANG ZHANG [République populaire de Chine] ; JUNJIE ZHANG [République populaire de Chine] ; LILI HU [République populaire de Chine]Source :
- Journal of non-crystalline solids [ 0022-3093 ] ; 2011.
Descripteurs français
- Pascal (Inist)
- Codopage, Transfert énergie, Addition thulium, Trempe état liquide, Théorie Judd Ofelt, Transition radiative, Durée vie radiative, Spectre absorption, Addition ytterbium, Addition lanthane, Spectre IR, Photoluminescence, Amplification optique, Système ternaire, Oxyde de zinc, Oxyde de bismuth, Verre de tellurite.
English descriptors
- KwdEn :
- Absorption spectra, Bismuth oxide, Codoping, Energy transfer, Infrared spectra, Judd-Ofelt theory, Lanthanum additions, Liquid state quenching, Optical amplification, Photoluminescence, Radiative lifetimes, Radiative transition, Tellurite glass, Ternary systems, Thulium additions, Ytterbium additions, Zinc oxide.
Abstract
Tm3+-doped and Tm3+/Yb3+-codoped TeO2-ZnO-Bi2O3 (TZB) glasses are prepared by melt-quenching method. The Judd-Ofelt intensity parameters (Ωt t = 2, 4, 6), radiative transition rate, and radiative lifetime of Tm3+ are calculated based on the absorption spectra. The 1.8 μm emission of the samples is investigated under 980 nm laser excitation. The absorption, emission cross-sections, and gain coefficient of Tm3+ :3F4 → 3H6 are calculated. The energy transfer processes of Yb3+-Yb3+ and Yb3+-Tm3+ are analyzed, the results show that the Yb3+ ions can transfer their energy to Tm3+ ions with large energy transfer coefficient, and a maximum efficiency of 79%.
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Links toward previous steps (curation, corpus...)
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Pascal:11-0327167Le document en format XML
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/Yb<sup>3+</sup>
codoped TeO<sub>2-</sub>
ZnO<sub>-</sub>
Bi<sub>2</sub>
O<sub>3</sub>
glasses with efficient energy transfer</title>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Spectroscopic properties of the 1.8 μm emission of Tm<sup>3+</sup>
/Yb<sup>3+</sup>
codoped TeO<sub>2-</sub>
ZnO<sub>-</sub>
Bi<sub>2</sub>
O<sub>3</sub>
glasses with efficient energy transfer</title>
<author><name sortKey="Kefeng Li" sort="Kefeng Li" uniqKey="Kefeng Li" last="Kefeng Li">KEFENG LI</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Graduate School of Chinese Academy of Sciences</s1>
<s2>Beijing 100039</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
</affiliation>
</author>
<author><name sortKey="Sijun Fan" sort="Sijun Fan" uniqKey="Sijun Fan" last="Sijun Fan">SIJUN FAN</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Graduate School of Chinese Academy of Sciences</s1>
<s2>Beijing 100039</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>République populaire de Chine</country>
</affiliation>
</author>
<author><name sortKey="Lei Zhang" sort="Lei Zhang" uniqKey="Lei Zhang" last="Lei Zhang">LEI ZHANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<country>République populaire de Chine</country>
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<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Graduate School of Chinese Academy of Sciences</s1>
<s2>Beijing 100039</s2>
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<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
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</affiliation>
</author>
<author><name sortKey="Qiang Zhang" sort="Qiang Zhang" uniqKey="Qiang Zhang" last="Qiang Zhang">QIANG ZHANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<sZ>3 aut.</sZ>
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</affiliation>
</author>
<author><name sortKey="Junjie Zhang" sort="Junjie Zhang" uniqKey="Junjie Zhang" last="Junjie Zhang">JUNJIE ZHANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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</affiliation>
</author>
<author><name sortKey="Lili Hu" sort="Lili Hu" uniqKey="Lili Hu" last="Lili Hu">LILI HU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
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</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Journal of non-crystalline solids</title>
<title level="j" type="abbreviated">J. non-cryst. solids</title>
<idno type="ISSN">0022-3093</idno>
<imprint><date when="2011">2011</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Journal of non-crystalline solids</title>
<title level="j" type="abbreviated">J. non-cryst. solids</title>
<idno type="ISSN">0022-3093</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectra</term>
<term>Bismuth oxide</term>
<term>Codoping</term>
<term>Energy transfer</term>
<term>Infrared spectra</term>
<term>Judd-Ofelt theory</term>
<term>Lanthanum additions</term>
<term>Liquid state quenching</term>
<term>Optical amplification</term>
<term>Photoluminescence</term>
<term>Radiative lifetimes</term>
<term>Radiative transition</term>
<term>Tellurite glass</term>
<term>Ternary systems</term>
<term>Thulium additions</term>
<term>Ytterbium additions</term>
<term>Zinc oxide</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Codopage</term>
<term>Transfert énergie</term>
<term>Addition thulium</term>
<term>Trempe état liquide</term>
<term>Théorie Judd Ofelt</term>
<term>Transition radiative</term>
<term>Durée vie radiative</term>
<term>Spectre absorption</term>
<term>Addition ytterbium</term>
<term>Addition lanthane</term>
<term>Spectre IR</term>
<term>Photoluminescence</term>
<term>Amplification optique</term>
<term>Système ternaire</term>
<term>Oxyde de zinc</term>
<term>Oxyde de bismuth</term>
<term>Verre de tellurite</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Tm<sup>3+</sup>
-doped and Tm<sup>3+</sup>
/Yb<sup>3+</sup>
-codoped TeO<sub>2-</sub>
ZnO<sub>-</sub>
Bi<sub>2</sub>
O<sub>3</sub>
(TZB) glasses are prepared by melt-quenching method. The Judd-Ofelt intensity parameters (Ω<sub>t</sub>
t = 2, 4, 6), radiative transition rate, and radiative lifetime of Tm<sup>3+</sup>
are calculated based on the absorption spectra. The 1.8 μm emission of the samples is investigated under 980 nm laser excitation. The absorption, emission cross-sections, and gain coefficient of Tm<sup>3+ </sup>
:<sup>3</sup>
F<sub>4</sub>
→ <sup>3</sup>
H<sub>6</sub>
are calculated. The energy transfer processes of Yb<sup>3+</sup>
-Yb<sup>3+</sup>
and Yb<sup>3+</sup>
<sub>-</sub>
Tm<sup>3+</sup>
are analyzed, the results show that the Yb<sup>3+</sup>
ions can transfer their energy to Tm<sup>3+</sup>
ions with large energy transfer coefficient, and a maximum efficiency of 79%.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-3093</s0>
</fA01>
<fA02 i1="01"><s0>JNCSBJ</s0>
</fA02>
<fA03 i2="1"><s0>J. non-cryst. solids</s0>
</fA03>
<fA05><s2>357</s2>
</fA05>
<fA06><s2>11-13</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Spectroscopic properties of the 1.8 μm emission of Tm<sup>3+</sup>
/Yb<sup>3+</sup>
codoped TeO<sub>2-</sub>
ZnO<sub>-</sub>
Bi<sub>2</sub>
O<sub>3</sub>
glasses with efficient energy transfer</s1>
</fA08>
<fA09 i1="01" i2="1" l="ENG"><s1>17th International Symposium on Non-Oxide and New Optical Glasses (XVII ISNOG), June 13-18, 2010, Ningbo, China</s1>
</fA09>
<fA11 i1="01" i2="1"><s1>KEFENG LI</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>SIJUN FAN</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>LEI ZHANG</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>QIANG ZHANG</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>JUNJIE ZHANG</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>LILI HU</s1>
</fA11>
<fA12 i1="01" i2="1"><s1>ZHANG (Long)</s1>
<s9>ed.</s9>
</fA12>
<fA12 i1="02" i2="1"><s1>QIU (Jianrong)</s1>
<s9>ed.</s9>
</fA12>
<fA14 i1="01"><s1>Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Graduate School of Chinese Academy of Sciences</s1>
<s2>Beijing 100039</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA15 i1="01"><s1>Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Science, P.O. Box 800-211</s1>
<s2>Shangai 201800</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
</fA15>
<fA15 i1="02"><s1>Zhejiang University</s1>
<s3>CHN</s3>
<sZ>2 aut.</sZ>
</fA15>
<fA18 i1="01" i2="1"><s1>Shanghai Institute of Optics and Fine Mechanics</s1>
<s2>Shangai 201800</s2>
<s3>CHN</s3>
<s9>org-cong.</s9>
</fA18>
<fA18 i1="02" i2="1"><s1>Ningbo University</s1>
<s2>Nigbo</s2>
<s3>CHN</s3>
<s9>org-cong.</s9>
</fA18>
<fA18 i1="03" i2="1"><s1>Chinese Academy of Science (CAS)</s1>
<s2>Beijing</s2>
<s3>CHN</s3>
<s9>org-cong.</s9>
</fA18>
<fA20><s1>2417-2420</s1>
</fA20>
<fA21><s1>2011</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14572</s2>
<s5>354000192186020500</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>15 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>11-0327167</s0>
</fA47>
<fA60><s1>P</s1>
<s2>C</s2>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Journal of non-crystalline solids</s0>
</fA64>
<fA66 i1="01"><s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Tm<sup>3+</sup>
-doped and Tm<sup>3+</sup>
/Yb<sup>3+</sup>
-codoped TeO<sub>2-</sub>
ZnO<sub>-</sub>
Bi<sub>2</sub>
O<sub>3</sub>
(TZB) glasses are prepared by melt-quenching method. The Judd-Ofelt intensity parameters (Ω<sub>t</sub>
t = 2, 4, 6), radiative transition rate, and radiative lifetime of Tm<sup>3+</sup>
are calculated based on the absorption spectra. The 1.8 μm emission of the samples is investigated under 980 nm laser excitation. The absorption, emission cross-sections, and gain coefficient of Tm<sup>3+ </sup>
:<sup>3</sup>
F<sub>4</sub>
→ <sup>3</sup>
H<sub>6</sub>
are calculated. The energy transfer processes of Yb<sup>3+</sup>
-Yb<sup>3+</sup>
and Yb<sup>3+</sup>
<sub>-</sub>
Tm<sup>3+</sup>
are analyzed, the results show that the Yb<sup>3+</sup>
ions can transfer their energy to Tm<sup>3+</sup>
ions with large energy transfer coefficient, and a maximum efficiency of 79%.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70H55Q</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Codopage</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Codoping</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Codrogado</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Transfert énergie</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Energy transfer</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Trempe état liquide</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Liquid state quenching</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Temple estado líquido</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Théorie Judd Ofelt</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Judd-Ofelt theory</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Transition radiative</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Radiative transition</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Transición radiativa</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Durée vie radiative</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Radiative lifetimes</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Spectre absorption</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Absorption spectra</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Addition ytterbium</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Ytterbium additions</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Addition lanthane</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Lanthanum additions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Spectre IR</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Infrared spectra</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Photoluminescence</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Photoluminescence</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Amplification optique</s0>
<s5>14</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Optical amplification</s0>
<s5>14</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Amplificación óptica</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Système ternaire</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Ternary systems</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE"><s0>Oxyde de zinc</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG"><s0>Zinc oxide</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA"><s0>Zinc óxido</s0>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>Oxyde de bismuth</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG"><s0>Bismuth oxide</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA"><s0>Bismuto óxido</s0>
<s5>17</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Verre de tellurite</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Tellurite glass</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="17" i2="3" l="SPA"><s0>Vidrio de telurito</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>220</s1>
</fN21>
</pA>
<pR><fA30 i1="01" i2="1" l="ENG"><s1>XVII ISNOG International Symposium on Non-Oxide and New Optical Glasses</s1>
<s2>17</s2>
<s3>Nigbo CHN</s3>
<s4>2010-06-13</s4>
</fA30>
</pR>
</standard>
</inist>
</record>
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