The energy transfer processes between the Er3+ and Tm3+ in Er, Tm-codoped-NaY(WO4)2 crystal
Identifieur interne : 000A06 ( Pascal/Corpus ); précédent : 000A05; suivant : 000A07The energy transfer processes between the Er3+ and Tm3+ in Er, Tm-codoped-NaY(WO4)2 crystal
Auteurs : FENG SONG ; JING SU ; HAO TAN ; LIN HAN ; BO FU ; JIANGUO TIAN ; GUANGYIN ZHANG ; ZHENXIANG CHENG ; HUANCHU CHENSource :
- Optics communications [ 0030-4018 ] ; 2004.
Descripteurs français
- Pascal (Inist)
- Niveau énergie, Matériau optique, Erbium III, Thulium III, Matériau dopé, Potassium Yttrium Tungstate, Transfert énergie, Croissance cristalline, Méthode Czochralski, Matériau laser, Spectrométrie absorption, Spectrométrie émission, Spectre excitation, Propriété optique, Température ambiante, Codopage, Addition erbium, Addition thulium, Transition optique, Etude expérimentale, NaY(WO4)2, Na O W Y, 4270H, 7855H.
English descriptors
- KwdEn :
- Absorption spectroscopy, Ambient temperature, Codoping, Crystal growth, Czochralski method, Doped materials, Emission spectroscopy, Energy levels, Energy transfer, Erbium III, Erbium additions, Excitation spectrum, Experimental study, Laser materials, Optical materials, Optical properties, Optical transition, Potassium Yttrium Tungstates, Thulium III, Thulium additions.
Abstract
Er3+,Tm3+-codoped NaY(WO4)2 crystal was prepared by using Czochralski (CZ) pulling method. Absorption spectra, emission spectra and excitation spectra of this crystal were measured at room temperature. Such optical parameters as intensity parameters, spontaneous emission probabilities, branch ratios and lifetimes are calculated from absorption spectra with Judd-Ofelt theory. Transition processes of the energy levels of Er3+, Tm3+ are analyzed in details and the cross-relaxations: 1G4(Tm3+) + 4I15/2(Er3+) → 3F2(Tm3+) + 4I13/2(Er3+). 1G4(Tm3+) + 4I15/2(Er3+) → 3F4(Tm3+) + 4F9/2(Er3+) and 3H4(Tm3+) + 4I9/2(Er3+) → 3F4(Tm3+) + 4S3/2(Er3+) or 2H11/2 between the two ions are put forward. Through the experiments, we have found that, in this crystal, Tm3+ strengthens luminescence of Er3+ in the green and red regions evidently. The above energy transfer processes provide potential applications of Tm3+ in Er3+-doped laser materials.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
pA |
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Format Inist (serveur)
NO : | PASCAL 05-0006568 INIST |
---|---|
ET : | The energy transfer processes between the Er3+ and Tm3+ in Er, Tm-codoped-NaY(WO4)2 crystal |
AU : | FENG SONG; JING SU; HAO TAN; LIN HAN; BO FU; JIANGUO TIAN; GUANGYIN ZHANG; ZHENXIANG CHENG; HUANCHU CHEN |
AF : | Photonics Center, College of Physics Sciences, Nankai University/Tianjin, 300071/Chine (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 6 aut., 7 aut.); Institute of Crystal, Shandong University/Jinan, Shandong Province/Chine (8 aut., 9 aut.) |
DT : | Publication en série; Niveau analytique |
SO : | Optics communications; ISSN 0030-4018; Coden OPCOB8; Pays-Bas; Da. 2004; Vol. 241; No. 4-6; Pp. 455-463; Bibl. 31 ref. |
LA : | Anglais |
EA : | Er3+,Tm3+-codoped NaY(WO4)2 crystal was prepared by using Czochralski (CZ) pulling method. Absorption spectra, emission spectra and excitation spectra of this crystal were measured at room temperature. Such optical parameters as intensity parameters, spontaneous emission probabilities, branch ratios and lifetimes are calculated from absorption spectra with Judd-Ofelt theory. Transition processes of the energy levels of Er3+, Tm3+ are analyzed in details and the cross-relaxations: 1G4(Tm3+) + 4I15/2(Er3+) → 3F2(Tm3+) + 4I13/2(Er3+). 1G4(Tm3+) + 4I15/2(Er3+) → 3F4(Tm3+) + 4F9/2(Er3+) and 3H4(Tm3+) + 4I9/2(Er3+) → 3F4(Tm3+) + 4S3/2(Er3+) or 2H11/2 between the two ions are put forward. Through the experiments, we have found that, in this crystal, Tm3+ strengthens luminescence of Er3+ in the green and red regions evidently. The above energy transfer processes provide potential applications of Tm3+ in Er3+-doped laser materials. |
CC : | 001B40B70H; 001B70H55H |
FD : | Niveau énergie; Matériau optique; Erbium III; Thulium III; Matériau dopé; Potassium Yttrium Tungstate; Transfert énergie; Croissance cristalline; Méthode Czochralski; Matériau laser; Spectrométrie absorption; Spectrométrie émission; Spectre excitation; Propriété optique; Température ambiante; Codopage; Addition erbium; Addition thulium; Transition optique; Etude expérimentale; NaY(WO4)2; Na O W Y; 4270H; 7855H |
ED : | Energy levels; Optical materials; Erbium III; Thulium III; Doped materials; Potassium Yttrium Tungstates; Energy transfer; Crystal growth; Czochralski method; Laser materials; Absorption spectroscopy; Emission spectroscopy; Excitation spectrum; Optical properties; Ambient temperature; Codoping; Erbium additions; Thulium additions; Optical transition; Experimental study |
SD : | Erbio III; Tulio III; Espectro excitación; Codrogado; Transición óptica |
LO : | INIST-14750.354000120499390280 |
ID : | 05-0006568 |
Links to Exploration step
Pascal:05-0006568Le document en format XML
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and Tm<sup>3+</sup>
in Er, Tm-codoped-NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal</title>
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<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
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<author><name sortKey="Zhenxiang Cheng" sort="Zhenxiang Cheng" uniqKey="Zhenxiang Cheng" last="Zhenxiang Cheng">ZHENXIANG CHENG</name>
<affiliation><inist:fA14 i1="02"><s1>Institute of Crystal, Shandong University</s1>
<s2>Jinan, Shandong Province</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
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<author><name sortKey="Huanchu Chen" sort="Huanchu Chen" uniqKey="Huanchu Chen" last="Huanchu Chen">HUANCHU CHEN</name>
<affiliation><inist:fA14 i1="02"><s1>Institute of Crystal, Shandong University</s1>
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<s3>CHN</s3>
<sZ>8 aut.</sZ>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">The energy transfer processes between the Er<sup>3+</sup>
and Tm<sup>3+</sup>
in Er, Tm-codoped-NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal</title>
<author><name sortKey="Feng Song" sort="Feng Song" uniqKey="Feng Song" last="Feng Song">FENG SONG</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Jing Su" sort="Jing Su" uniqKey="Jing Su" last="Jing Su">JING SU</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Hao Tan" sort="Hao Tan" uniqKey="Hao Tan" last="Hao Tan">HAO TAN</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Lin Han" sort="Lin Han" uniqKey="Lin Han" last="Lin Han">LIN HAN</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Bo Fu" sort="Bo Fu" uniqKey="Bo Fu" last="Bo Fu">BO FU</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Jianguo Tian" sort="Jianguo Tian" uniqKey="Jianguo Tian" last="Jianguo Tian">JIANGUO TIAN</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Guangyin Zhang" sort="Guangyin Zhang" uniqKey="Guangyin Zhang" last="Guangyin Zhang">GUANGYIN ZHANG</name>
<affiliation><inist:fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<sZ>5 aut.</sZ>
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</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Zhenxiang Cheng" sort="Zhenxiang Cheng" uniqKey="Zhenxiang Cheng" last="Zhenxiang Cheng">ZHENXIANG CHENG</name>
<affiliation><inist:fA14 i1="02"><s1>Institute of Crystal, Shandong University</s1>
<s2>Jinan, Shandong Province</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Huanchu Chen" sort="Huanchu Chen" uniqKey="Huanchu Chen" last="Huanchu Chen">HUANCHU CHEN</name>
<affiliation><inist:fA14 i1="02"><s1>Institute of Crystal, Shandong University</s1>
<s2>Jinan, Shandong Province</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Optics communications</title>
<title level="j" type="abbreviated">Opt. commun.</title>
<idno type="ISSN">0030-4018</idno>
<imprint><date when="2004">2004</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Optics communications</title>
<title level="j" type="abbreviated">Opt. commun.</title>
<idno type="ISSN">0030-4018</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectroscopy</term>
<term>Ambient temperature</term>
<term>Codoping</term>
<term>Crystal growth</term>
<term>Czochralski method</term>
<term>Doped materials</term>
<term>Emission spectroscopy</term>
<term>Energy levels</term>
<term>Energy transfer</term>
<term>Erbium III</term>
<term>Erbium additions</term>
<term>Excitation spectrum</term>
<term>Experimental study</term>
<term>Laser materials</term>
<term>Optical materials</term>
<term>Optical properties</term>
<term>Optical transition</term>
<term>Potassium Yttrium Tungstates</term>
<term>Thulium III</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Niveau énergie</term>
<term>Matériau optique</term>
<term>Erbium III</term>
<term>Thulium III</term>
<term>Matériau dopé</term>
<term>Potassium Yttrium Tungstate</term>
<term>Transfert énergie</term>
<term>Croissance cristalline</term>
<term>Méthode Czochralski</term>
<term>Matériau laser</term>
<term>Spectrométrie absorption</term>
<term>Spectrométrie émission</term>
<term>Spectre excitation</term>
<term>Propriété optique</term>
<term>Température ambiante</term>
<term>Codopage</term>
<term>Addition erbium</term>
<term>Addition thulium</term>
<term>Transition optique</term>
<term>Etude expérimentale</term>
<term>NaY(WO4)2</term>
<term>Na O W Y</term>
<term>4270H</term>
<term>7855H</term>
</keywords>
</textClass>
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</teiHeader>
<front><div type="abstract" xml:lang="en">Er<sup>3+</sup>
,Tm<sup>3+</sup>
-codoped NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal was prepared by using Czochralski (CZ) pulling method. Absorption spectra, emission spectra and excitation spectra of this crystal were measured at room temperature. Such optical parameters as intensity parameters, spontaneous emission probabilities, branch ratios and lifetimes are calculated from absorption spectra with Judd-Ofelt theory. Transition processes of the energy levels of Er<sup>3+</sup>
, Tm<sup>3+</sup>
are analyzed in details and the cross-relaxations: <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>2</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>13/2</sub>
(Er<sup>3+</sup>
). <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
F<sub>9/2</sub>
(Er<sup>3+</sup>
) and <sup>3</sup>
H<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>9/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
S<sub>3/2</sub>
(Er<sup>3+</sup>
) or <sup>2</sup>
H<sub>11/2</sub>
between the two ions are put forward. Through the experiments, we have found that, in this crystal, Tm<sup>3+</sup>
strengthens luminescence of Er<sup>3+</sup>
in the green and red regions evidently. The above energy transfer processes provide potential applications of Tm<sup>3+</sup>
in Er<sup>3+</sup>
-doped laser materials.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0030-4018</s0>
</fA01>
<fA02 i1="01"><s0>OPCOB8</s0>
</fA02>
<fA03 i2="1"><s0>Opt. commun.</s0>
</fA03>
<fA05><s2>241</s2>
</fA05>
<fA06><s2>4-6</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>The energy transfer processes between the Er<sup>3+</sup>
and Tm<sup>3+</sup>
in Er, Tm-codoped-NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>FENG SONG</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>JING SU</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>HAO TAN</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>LIN HAN</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>BO FU</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>JIANGUO TIAN</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>GUANGYIN ZHANG</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>ZHENXIANG CHENG</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>HUANCHU CHEN</s1>
</fA11>
<fA14 i1="01"><s1>Photonics Center, College of Physics Sciences, Nankai University</s1>
<s2>Tianjin, 300071</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>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Institute of Crystal, Shandong University</s1>
<s2>Jinan, Shandong Province</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA20><s1>455-463</s1>
</fA20>
<fA21><s1>2004</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14750</s2>
<s5>354000120499390280</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2005 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>31 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>05-0006568</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Optics communications</s0>
</fA64>
<fA66 i1="01"><s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Er<sup>3+</sup>
,Tm<sup>3+</sup>
-codoped NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal was prepared by using Czochralski (CZ) pulling method. Absorption spectra, emission spectra and excitation spectra of this crystal were measured at room temperature. Such optical parameters as intensity parameters, spontaneous emission probabilities, branch ratios and lifetimes are calculated from absorption spectra with Judd-Ofelt theory. Transition processes of the energy levels of Er<sup>3+</sup>
, Tm<sup>3+</sup>
are analyzed in details and the cross-relaxations: <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>2</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>13/2</sub>
(Er<sup>3+</sup>
). <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
F<sub>9/2</sub>
(Er<sup>3+</sup>
) and <sup>3</sup>
H<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>9/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
S<sub>3/2</sub>
(Er<sup>3+</sup>
) or <sup>2</sup>
H<sub>11/2</sub>
between the two ions are put forward. Through the experiments, we have found that, in this crystal, Tm<sup>3+</sup>
strengthens luminescence of Er<sup>3+</sup>
in the green and red regions evidently. The above energy transfer processes provide potential applications of Tm<sup>3+</sup>
in Er<sup>3+</sup>
-doped laser materials.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B70H</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B70H55H</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Niveau énergie</s0>
<s5>45</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Energy levels</s0>
<s5>45</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Matériau optique</s0>
<s5>50</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Optical materials</s0>
<s5>50</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE"><s0>Erbium III</s0>
<s2>NC</s2>
<s5>51</s5>
<s6>Erbium «III»</s6>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Erbium III</s0>
<s2>NC</s2>
<s5>51</s5>
<s6>Erbium «III»</s6>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Erbio III</s0>
<s2>NC</s2>
<s5>51</s5>
<s6>Erbio «III»</s6>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Thulium III</s0>
<s2>NC</s2>
<s5>52</s5>
<s6>Thulium «III»</s6>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Thulium III</s0>
<s2>NC</s2>
<s5>52</s5>
<s6>Thulium «III»</s6>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Tulio III</s0>
<s2>NC</s2>
<s5>52</s5>
<s6>Tulio «III»</s6>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>53</s5>
<s6>Matériau dopé</s6>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>53</s5>
<s6>Doped materials</s6>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Potassium Yttrium Tungstate</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>54</s5>
<s6>Potassium Yttrium Tungstate</s6>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Potassium Yttrium Tungstates</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>54</s5>
<s6>Potassium Yttrium Tungstates</s6>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Transfert énergie</s0>
<s5>55</s5>
<s6>Transfert énergie</s6>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Energy transfer</s0>
<s5>55</s5>
<s6>Energy transfer</s6>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Croissance cristalline</s0>
<s5>56</s5>
<s6>Croissance cristalline</s6>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Crystal growth</s0>
<s5>56</s5>
<s6>Crystal growth</s6>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Méthode Czochralski</s0>
<s5>57</s5>
<s6>Méthode Czochralski</s6>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Czochralski method</s0>
<s5>57</s5>
<s6>Czochralski method</s6>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Matériau laser</s0>
<s5>58</s5>
<s6>Matériau laser</s6>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Laser materials</s0>
<s5>58</s5>
<s6>Laser materials</s6>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Spectrométrie absorption</s0>
<s5>59</s5>
<s6>Spectrométrie absorption</s6>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Absorption spectroscopy</s0>
<s5>59</s5>
<s6>Absorption spectroscopy</s6>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Spectrométrie émission</s0>
<s5>60</s5>
<s6>Spectrométrie émission</s6>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Emission spectroscopy</s0>
<s5>60</s5>
<s6>Emission spectroscopy</s6>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Spectre excitation</s0>
<s5>61</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Excitation spectrum</s0>
<s5>61</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Espectro excitación</s0>
<s5>61</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Propriété optique</s0>
<s5>62</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Optical properties</s0>
<s5>62</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Température ambiante</s0>
<s5>63</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Ambient temperature</s0>
<s5>63</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>Codopage</s0>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG"><s0>Codoping</s0>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA"><s0>Codrogado</s0>
<s5>65</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Addition erbium</s0>
<s5>66</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Erbium additions</s0>
<s5>66</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>67</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>67</s5>
</fC03>
<fC03 i1="19" i2="X" l="FRE"><s0>Transition optique</s0>
<s5>68</s5>
</fC03>
<fC03 i1="19" i2="X" l="ENG"><s0>Optical transition</s0>
<s5>68</s5>
</fC03>
<fC03 i1="19" i2="X" l="SPA"><s0>Transición óptica</s0>
<s5>68</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>69</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>69</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>NaY(WO4)2</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>Na O W Y</s0>
<s4>INC</s4>
<s5>76</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>4270H</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="24" i2="3" l="FRE"><s0>7855H</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fN21><s1>004</s1>
</fN21>
<fN44 i1="01"><s1>PSI</s1>
</fN44>
<fN82><s1>PSI</s1>
</fN82>
</pA>
</standard>
<server><NO>PASCAL 05-0006568 INIST</NO>
<ET>The energy transfer processes between the Er<sup>3+</sup>
and Tm<sup>3+</sup>
in Er, Tm-codoped-NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal</ET>
<AU>FENG SONG; JING SU; HAO TAN; LIN HAN; BO FU; JIANGUO TIAN; GUANGYIN ZHANG; ZHENXIANG CHENG; HUANCHU CHEN</AU>
<AF>Photonics Center, College of Physics Sciences, Nankai University/Tianjin, 300071/Chine (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 6 aut., 7 aut.); Institute of Crystal, Shandong University/Jinan, Shandong Province/Chine (8 aut., 9 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Optics communications; ISSN 0030-4018; Coden OPCOB8; Pays-Bas; Da. 2004; Vol. 241; No. 4-6; Pp. 455-463; Bibl. 31 ref.</SO>
<LA>Anglais</LA>
<EA>Er<sup>3+</sup>
,Tm<sup>3+</sup>
-codoped NaY(WO<sub>4</sub>
)<sub>2</sub>
crystal was prepared by using Czochralski (CZ) pulling method. Absorption spectra, emission spectra and excitation spectra of this crystal were measured at room temperature. Such optical parameters as intensity parameters, spontaneous emission probabilities, branch ratios and lifetimes are calculated from absorption spectra with Judd-Ofelt theory. Transition processes of the energy levels of Er<sup>3+</sup>
, Tm<sup>3+</sup>
are analyzed in details and the cross-relaxations: <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>2</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>13/2</sub>
(Er<sup>3+</sup>
). <sup>1</sup>
G<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>15/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
F<sub>9/2</sub>
(Er<sup>3+</sup>
) and <sup>3</sup>
H<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
I<sub>9/2</sub>
(Er<sup>3+</sup>
) → <sup>3</sup>
F<sub>4</sub>
(Tm<sup>3+</sup>
) + <sup>4</sup>
S<sub>3/2</sub>
(Er<sup>3+</sup>
) or <sup>2</sup>
H<sub>11/2</sub>
between the two ions are put forward. Through the experiments, we have found that, in this crystal, Tm<sup>3+</sup>
strengthens luminescence of Er<sup>3+</sup>
in the green and red regions evidently. The above energy transfer processes provide potential applications of Tm<sup>3+</sup>
in Er<sup>3+</sup>
-doped laser materials.</EA>
<CC>001B40B70H; 001B70H55H</CC>
<FD>Niveau énergie; Matériau optique; Erbium III; Thulium III; Matériau dopé; Potassium Yttrium Tungstate; Transfert énergie; Croissance cristalline; Méthode Czochralski; Matériau laser; Spectrométrie absorption; Spectrométrie émission; Spectre excitation; Propriété optique; Température ambiante; Codopage; Addition erbium; Addition thulium; Transition optique; Etude expérimentale; NaY(WO4)2; Na O W Y; 4270H; 7855H</FD>
<ED>Energy levels; Optical materials; Erbium III; Thulium III; Doped materials; Potassium Yttrium Tungstates; Energy transfer; Crystal growth; Czochralski method; Laser materials; Absorption spectroscopy; Emission spectroscopy; Excitation spectrum; Optical properties; Ambient temperature; Codoping; Erbium additions; Thulium additions; Optical transition; Experimental study</ED>
<SD>Erbio III; Tulio III; Espectro excitación; Codrogado; Transición óptica</SD>
<LO>INIST-14750.354000120499390280</LO>
<ID>05-0006568</ID>
</server>
</inist>
</record>
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