Spectroscopic properties of Tm3+ doped TeO2-R2O-La2O3 glasses for 1.47 μm optical amplifiers
Identifieur interne :
000234 ( Pascal/Curation );
précédent :
000233;
suivant :
000235
Spectroscopic properties of Tm3+ doped TeO2-R2O-La2O3 glasses for 1.47 μm optical amplifiers
Auteurs : DACHENG ZHOU [
République populaire de Chine] ;
RONGFEI WANG [
République populaire de Chine] ;
ZHENGWEN YANG [
République populaire de Chine] ;
ZHIGUO SONG [
République populaire de Chine] ;
ZHAOYI YIN [
République populaire de Chine] ;
JIANBEI QIU [
République populaire de Chine]
Source :
-
Journal of non-crystalline solids [ 0022-3093 ] ; 2011.
RBID : Pascal:11-0327164
Descripteurs français
- Pascal (Inist)
- Dopage,
Addition thulium,
Fluorescence,
Théorie Judd Ofelt,
Largeur bande,
Rapport branchement,
Spectre absorption,
Amplification optique,
Système ternaire,
Oxyde de lanthane,
Verre fluorure,
Oxyde de potassium,
Oxyde de lithium,
Oxyde de sodium,
Verre de tellurite.
- Wicri :
English descriptors
- KwdEn :
- Absorption spectra,
Bandwidth,
Branching ratio,
Doping,
Fluorescence,
Fluoride glass,
Judd-Ofelt theory,
Lanthanum oxide,
Lithium oxide,
Optical amplification,
Potassium oxide,
Sodium oxide,
Tellurite glass,
Ternary systems,
Thulium additions.
Abstract
Upon excitation at 808 nm laser diode, an intense 1.47 μm infrared fluorescence has been observed with a broad full width at half maximum (FWHM) of about 124 nm for the Tm3+-doped TeO2-K2O-La2O3 glass. The Judd-Ofelt parameters found for this glass are: Ω2 = 5.26 × 10-20 cm2, Ω4 = 1.57 × 10-20 cm2 and Ω6 = 1.44 × 10-20 cm2. The calculated emission cross-sections of the 1.47 μm transition are 3.57 x 10-21 cm2, respectively. It is noted that the gain bandwidth, σe × FWHM, of the glass is about 440 x 10-28 cm3, which is significantly higher than that in ZBLAN and Gallate glasses, a high gain of 35.5 dB at 1470 nm can be obtained in a TKLglass fiber. TeO2-R2O ( R= Li, Na, K)-La2O3 glasses has been considered to be more useful as a host for broadband optical fiber amplifier.
| pA |
| A01 | 01 | 1 | | @0 0022-3093 |
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| A02 | 01 | | | @0 JNCSBJ |
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| A03 | | 1 | | @0 J. non-cryst. solids |
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| A05 | | | | @2 357 |
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| A06 | | | | @2 11-13 |
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| A08 | 01 | 1 | ENG | @1 Spectroscopic properties of Tm3+ doped TeO2-R2O-La2O3 glasses for 1.47 μm optical amplifiers |
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| A09 | 01 | 1 | ENG | @1 17th International Symposium on Non-Oxide and New Optical Glasses (XVII ISNOG), June 13-18, 2010, Ningbo, China |
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| A11 | 01 | 1 | | @1 DACHENG ZHOU |
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| A11 | 02 | 1 | | @1 RONGFEI WANG |
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| A11 | 03 | 1 | | @1 ZHENGWEN YANG |
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| A11 | 04 | 1 | | @1 ZHIGUO SONG |
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| A11 | 05 | 1 | | @1 ZHAOYI YIN |
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| A11 | 06 | 1 | | @1 JIANBEI QIU |
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| A12 | 01 | 1 | | @1 ZHANG (Long) @9 ed. |
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| A12 | 02 | 1 | | @1 QIU (Jianrong) @9 ed. |
|---|
| A14 | 01 | | | @1 Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD @2 Kunming 650093 @3 CHN @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut. |
|---|
| A15 | 01 | | | @1 Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Science, P.O. Box 800-211 @2 Shangai 201800 @3 CHN @Z 1 aut. |
|---|
| A15 | 02 | | | @1 Zhejiang University @3 CHN @Z 2 aut. |
|---|
| A18 | 01 | 1 | | @1 Shanghai Institute of Optics and Fine Mechanics @2 Shangai 201800 @3 CHN @9 org-cong. |
|---|
| A18 | 02 | 1 | | @1 Ningbo University @2 Nigbo @3 CHN @9 org-cong. |
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| A18 | 03 | 1 | | @1 Chinese Academy of Science (CAS) @2 Beijing @3 CHN @9 org-cong. |
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| A20 | | | | @1 2409-2412 |
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| A21 | | | | @1 2011 |
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| A23 | 01 | | | @0 ENG |
|---|
| A43 | 01 | | | @1 INIST @2 14572 @5 354000192186020480 |
|---|
| A44 | | | | @0 0000 @1 © 2011 INIST-CNRS. All rights reserved. |
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| A45 | | | | @0 25 ref. |
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| A47 | 01 | 1 | | @0 11-0327164 |
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| A60 | | | | @1 P @2 C |
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| A61 | | | | @0 A |
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| A64 | 01 | 1 | | @0 Journal of non-crystalline solids |
|---|
| A66 | 01 | | | @0 GBR |
|---|
| C01 | 01 | | ENG | @0 Upon excitation at 808 nm laser diode, an intense 1.47 μm infrared fluorescence has been observed with a broad full width at half maximum (FWHM) of about 124 nm for the Tm3+-doped TeO2-K2O-La2O3 glass. The Judd-Ofelt parameters found for this glass are: Ω2 = 5.26 × 10-20 cm2, Ω4 = 1.57 × 10-20 cm2 and Ω6 = 1.44 × 10-20 cm2. The calculated emission cross-sections of the 1.47 μm transition are 3.57 x 10-21 cm2, respectively. It is noted that the gain bandwidth, σe × FWHM, of the glass is about 440 x 10-28 cm3, which is significantly higher than that in ZBLAN and Gallate glasses, a high gain of 35.5 dB at 1470 nm can be obtained in a TKLglass fiber. TeO2-R2O ( R= Li, Na, K)-La2O3 glasses has been considered to be more useful as a host for broadband optical fiber amplifier. |
|---|
| C02 | 01 | 3 | | @0 001B70H55Q |
|---|
| C03 | 01 | X | FRE | @0 Dopage @5 02 |
|---|
| C03 | 01 | X | ENG | @0 Doping @5 02 |
|---|
| C03 | 01 | X | SPA | @0 Doping @5 02 |
|---|
| C03 | 02 | 3 | FRE | @0 Addition thulium @5 03 |
|---|
| C03 | 02 | 3 | ENG | @0 Thulium additions @5 03 |
|---|
| C03 | 03 | 3 | FRE | @0 Fluorescence @5 04 |
|---|
| C03 | 03 | 3 | ENG | @0 Fluorescence @5 04 |
|---|
| C03 | 04 | 3 | FRE | @0 Théorie Judd Ofelt @5 05 |
|---|
| C03 | 04 | 3 | ENG | @0 Judd-Ofelt theory @5 05 |
|---|
| C03 | 05 | 3 | FRE | @0 Largeur bande @5 06 |
|---|
| C03 | 05 | 3 | ENG | @0 Bandwidth @5 06 |
|---|
| C03 | 06 | 3 | FRE | @0 Rapport branchement @5 07 |
|---|
| C03 | 06 | 3 | ENG | @0 Branching ratio @5 07 |
|---|
| C03 | 07 | 3 | FRE | @0 Spectre absorption @5 08 |
|---|
| C03 | 07 | 3 | ENG | @0 Absorption spectra @5 08 |
|---|
| C03 | 08 | X | FRE | @0 Amplification optique @5 11 |
|---|
| C03 | 08 | X | ENG | @0 Optical amplification @5 11 |
|---|
| C03 | 08 | X | SPA | @0 Amplificación óptica @5 11 |
|---|
| C03 | 09 | 3 | FRE | @0 Système ternaire @5 15 |
|---|
| C03 | 09 | 3 | ENG | @0 Ternary systems @5 15 |
|---|
| C03 | 10 | X | FRE | @0 Oxyde de lanthane @5 16 |
|---|
| C03 | 10 | X | ENG | @0 Lanthanum oxide @5 16 |
|---|
| C03 | 10 | X | SPA | @0 Lantano óxido @5 16 |
|---|
| C03 | 11 | 3 | FRE | @0 Verre fluorure @5 17 |
|---|
| C03 | 11 | 3 | ENG | @0 Fluoride glass @5 17 |
|---|
| C03 | 12 | X | FRE | @0 Oxyde de potassium @5 18 |
|---|
| C03 | 12 | X | ENG | @0 Potassium oxide @5 18 |
|---|
| C03 | 12 | X | SPA | @0 Potasio óxido @5 18 |
|---|
| C03 | 13 | X | FRE | @0 Oxyde de lithium @5 19 |
|---|
| C03 | 13 | X | ENG | @0 Lithium oxide @5 19 |
|---|
| C03 | 13 | X | SPA | @0 Litio óxido @5 19 |
|---|
| C03 | 14 | X | FRE | @0 Oxyde de sodium @5 20 |
|---|
| C03 | 14 | X | ENG | @0 Sodium oxide @5 20 |
|---|
| C03 | 14 | X | SPA | @0 Sodio óxido @5 20 |
|---|
| C03 | 15 | 3 | FRE | @0 Verre de tellurite @4 CD @5 96 |
|---|
| C03 | 15 | 3 | ENG | @0 Tellurite glass @4 CD @5 96 |
|---|
| C03 | 15 | 3 | SPA | @0 Vidrio de telurito @4 CD @5 96 |
|---|
| N21 | | | | @1 220 |
|---|
|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 XVII ISNOG International Symposium on Non-Oxide and New Optical Glasses @2 17 @3 Nigbo CHN @4 2010-06-13 |
|---|
|
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Le document en format XML
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doped TeO<sub>2</sub>
-R<sub>2</sub>
O-La<sub>2</sub>
O<sub>3</sub>
glasses for 1.47 μm optical amplifiers</title><author><name sortKey="Dacheng Zhou" sort="Dacheng Zhou" uniqKey="Dacheng Zhou" last="Dacheng Zhou">DACHENG ZHOU</name>
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<s2>Kunming 650093</s2>
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<date when="2011">2011</date>
<idno type="stanalyst">PASCAL 11-0327164 INIST</idno>
<idno type="RBID">Pascal:11-0327164</idno>
<idno type="wicri:Area/Pascal/Corpus">000234</idno>
<idno type="wicri:Area/Pascal/Curation">000234</idno>
</publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Spectroscopic properties of Tm<sup>3+</sup>
doped TeO<sub>2</sub>
-R<sub>2</sub>
O-La<sub>2</sub>
O<sub>3</sub>
glasses for 1.47 μm optical amplifiers</title><author><name sortKey="Dacheng Zhou" sort="Dacheng Zhou" uniqKey="Dacheng Zhou" last="Dacheng Zhou">DACHENG ZHOU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><author><name sortKey="Rongfei Wang" sort="Rongfei Wang" uniqKey="Rongfei Wang" last="Rongfei Wang">RONGFEI WANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><author><name sortKey="Zhengwen Yang" sort="Zhengwen Yang" uniqKey="Zhengwen Yang" last="Zhengwen Yang">ZHENGWEN YANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><author><name sortKey="Zhiguo Song" sort="Zhiguo Song" uniqKey="Zhiguo Song" last="Zhiguo Song">ZHIGUO SONG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><author><name sortKey="Zhaoyi Yin" sort="Zhaoyi Yin" uniqKey="Zhaoyi Yin" last="Zhaoyi Yin">ZHAOYI YIN</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><author><name sortKey="Jianbei Qiu" sort="Jianbei Qiu" uniqKey="Jianbei Qiu" last="Jianbei Qiu">JIANBEI QIU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><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><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><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectra</term>
<term>Bandwidth</term>
<term>Branching ratio</term>
<term>Doping</term>
<term>Fluorescence</term>
<term>Fluoride glass</term>
<term>Judd-Ofelt theory</term>
<term>Lanthanum oxide</term>
<term>Lithium oxide</term>
<term>Optical amplification</term>
<term>Potassium oxide</term>
<term>Sodium oxide</term>
<term>Tellurite glass</term>
<term>Ternary systems</term>
<term>Thulium additions</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Dopage</term>
<term>Addition thulium</term>
<term>Fluorescence</term>
<term>Théorie Judd Ofelt</term>
<term>Largeur bande</term>
<term>Rapport branchement</term>
<term>Spectre absorption</term>
<term>Amplification optique</term>
<term>Système ternaire</term>
<term>Oxyde de lanthane</term>
<term>Verre fluorure</term>
<term>Oxyde de potassium</term>
<term>Oxyde de lithium</term>
<term>Oxyde de sodium</term>
<term>Verre de tellurite</term>
</keywords><keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Dopage</term>
</keywords><front><div type="abstract" xml:lang="en">Upon excitation at 808 nm laser diode, an intense 1.47 μm infrared fluorescence has been observed with a broad full width at half maximum (FWHM) of about 124 nm for the Tm<sup>3+</sup>
-doped TeO<sub>2</sub>
-K<sub>2</sub>
O-La<sub>2</sub>
O<sub>3</sub>
glass. The Judd-Ofelt parameters found for this glass are: Ω<sub>2</sub>
= 5.26 × 10<sup>-20</sup>
cm<sup>2</sup>
, Ω<sub>4</sub>
= 1.57 × 10<sup>-20</sup>
cm<sup>2</sup>
and Ω<sub>6</sub>
= 1.44 × 10<sup>-20</sup>
cm<sup>2</sup>
. The calculated emission cross-sections of the 1.47 μm transition are 3.57 x 10<sup>-21</sup>
cm<sup>2</sup>
, respectively. It is noted that the gain bandwidth, σ<sub>e</sub>
× FWHM, of the glass is about 440 x 10<sup>-28</sup>
cm<sup>3</sup>
, which is significantly higher than that in ZBLAN and Gallate glasses, a high gain of 35.5 dB at 1470 nm can be obtained in a TKLglass fiber. TeO<sub>2</sub>
-R<sub>2</sub>
O ( R= Li, Na, K)-La<sub>2</sub>
O<sub>3</sub>
glasses has been considered to be more useful as a host for broadband optical fiber amplifier.</div><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 Tm<sup>3+</sup>
doped TeO<sub>2</sub>
-R<sub>2</sub>
O-La<sub>2</sub>
O<sub>3</sub>
glasses for 1.47 μm optical amplifiers</s1><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>DACHENG ZHOU</s1>
</fA11><fA11 i1="02" i2="1"><s1>RONGFEI WANG</s1>
</fA11><fA11 i1="03" i2="1"><s1>ZHENGWEN YANG</s1>
</fA11><fA11 i1="04" i2="1"><s1>ZHIGUO SONG</s1>
</fA11><fA11 i1="05" i2="1"><s1>ZHAOYI YIN</s1>
</fA11><fA11 i1="06" i2="1"><s1>JIANBEI QIU</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>Faculty of Material Science and Engineering, Kunming University of Science and Technology, Xuefu RD</s1>
<s2>Kunming 650093</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><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>2409-2412</s1>
</fA20><fA21><s1>2011</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA43 i1="01"><s1>INIST</s1>
<s2>14572</s2>
<s5>354000192186020480</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>25 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>11-0327164</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><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>Upon excitation at 808 nm laser diode, an intense 1.47 μm infrared fluorescence has been observed with a broad full width at half maximum (FWHM) of about 124 nm for the Tm<sup>3+</sup>
-doped TeO<sub>2</sub>
-K<sub>2</sub>
O-La<sub>2</sub>
O<sub>3</sub>
glass. The Judd-Ofelt parameters found for this glass are: Ω<sub>2</sub>
= 5.26 × 10<sup>-20</sup>
cm<sup>2</sup>
, Ω<sub>4</sub>
= 1.57 × 10<sup>-20</sup>
cm<sup>2</sup>
and Ω<sub>6</sub>
= 1.44 × 10<sup>-20</sup>
cm<sup>2</sup>
. The calculated emission cross-sections of the 1.47 μm transition are 3.57 x 10<sup>-21</sup>
cm<sup>2</sup>
, respectively. It is noted that the gain bandwidth, σ<sub>e</sub>
× FWHM, of the glass is about 440 x 10<sup>-28</sup>
cm<sup>3</sup>
, which is significantly higher than that in ZBLAN and Gallate glasses, a high gain of 35.5 dB at 1470 nm can be obtained in a TKLglass fiber. TeO<sub>2</sub>
-R<sub>2</sub>
O ( R= Li, Na, K)-La<sub>2</sub>
O<sub>3</sub>
glasses has been considered to be more useful as a host for broadband optical fiber amplifier.</s0><fC02 i1="01" i2="3"><s0>001B70H55Q</s0>
</fC02><fC03 i1="01" i2="X" l="FRE"><s0>Dopage</s0>
<s5>02</s5>
</fC03><fC03 i1="01" i2="X" l="ENG"><s0>Doping</s0>
<s5>02</s5>
</fC03><fC03 i1="01" i2="X" l="SPA"><s0>Doping</s0>
<s5>02</s5>
</fC03><fC03 i1="02" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>03</s5>
</fC03><fC03 i1="02" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Fluorescence</s0>
<s5>04</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>Fluorescence</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="3" l="FRE"><s0>Théorie Judd Ofelt</s0>
<s5>05</s5>
</fC03><fC03 i1="04" i2="3" l="ENG"><s0>Judd-Ofelt theory</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Largeur bande</s0>
<s5>06</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Bandwidth</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="3" l="FRE"><s0>Rapport branchement</s0>
<s5>07</s5>
</fC03><fC03 i1="06" i2="3" l="ENG"><s0>Branching ratio</s0>
<s5>07</s5>
</fC03><fC03 i1="07" i2="3" l="FRE"><s0>Spectre absorption</s0>
<s5>08</s5>
</fC03><fC03 i1="07" i2="3" l="ENG"><s0>Absorption spectra</s0>
<s5>08</s5>
</fC03><fC03 i1="08" i2="X" l="FRE"><s0>Amplification optique</s0>
<s5>11</s5>
</fC03><fC03 i1="08" i2="X" l="ENG"><s0>Optical amplification</s0>
<s5>11</s5>
</fC03><fC03 i1="08" i2="X" l="SPA"><s0>Amplificación óptica</s0>
<s5>11</s5>
</fC03><fC03 i1="09" i2="3" l="FRE"><s0>Système ternaire</s0>
<s5>15</s5>
</fC03><fC03 i1="09" i2="3" l="ENG"><s0>Ternary systems</s0>
<s5>15</s5>
</fC03><fC03 i1="10" i2="X" l="FRE"><s0>Oxyde de lanthane</s0>
<s5>16</s5>
</fC03><fC03 i1="10" i2="X" l="ENG"><s0>Lanthanum oxide</s0>
<s5>16</s5>
</fC03><fC03 i1="10" i2="X" l="SPA"><s0>Lantano óxido</s0>
<s5>16</s5>
</fC03><fC03 i1="11" i2="3" l="FRE"><s0>Verre fluorure</s0>
<s5>17</s5>
</fC03><fC03 i1="11" i2="3" l="ENG"><s0>Fluoride glass</s0>
<s5>17</s5>
</fC03><fC03 i1="12" i2="X" l="FRE"><s0>Oxyde de potassium</s0>
<s5>18</s5>
</fC03><fC03 i1="12" i2="X" l="ENG"><s0>Potassium oxide</s0>
<s5>18</s5>
</fC03><fC03 i1="12" i2="X" l="SPA"><s0>Potasio óxido</s0>
<s5>18</s5>
</fC03><fC03 i1="13" i2="X" l="FRE"><s0>Oxyde de lithium</s0>
<s5>19</s5>
</fC03><fC03 i1="13" i2="X" l="ENG"><s0>Lithium oxide</s0>
<s5>19</s5>
</fC03><fC03 i1="13" i2="X" l="SPA"><s0>Litio óxido</s0>
<s5>19</s5>
</fC03><fC03 i1="14" i2="X" l="FRE"><s0>Oxyde de sodium</s0>
<s5>20</s5>
</fC03><fC03 i1="14" i2="X" l="ENG"><s0>Sodium oxide</s0>
<s5>20</s5>
</fC03><fC03 i1="14" i2="X" l="SPA"><s0>Sodio óxido</s0>
<s5>20</s5>
</fC03><fC03 i1="15" i2="3" l="FRE"><s0>Verre de tellurite</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03><fC03 i1="15" i2="3" l="ENG"><s0>Tellurite glass</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03><fC03 i1="15" i2="3" l="SPA"><s0>Vidrio de telurito</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03><fN21><s1>220</s1>
</fN21><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>
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