ThuliumV1, Pascal, Curation, bibRecord, 000617

Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers

Identifieur interne : 000617 ( Pascal/Curation ); précédent : 000616; suivant : 000618

Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers

Auteurs : XINGHUA MA [République populaire de Chine] ; JIANFU LI [République populaire de Chine] ; ZHAOJIE ZHU [République populaire de Chine] ; ZHENYU YOU [République populaire de Chine] ; YAN WANG [République populaire de Chine] ; CHAOYANG TU [République populaire de Chine]

Source :

Journal of luminescence [ 0022-2313 ] ; 2008.

RBID : Pascal:08-0399143

Descripteurs français

Pascal (Inist)
- Propriété thermique, Dopage, Méthode Czochralski, Chaleur massique, Spectre absorption, Théorie Judd Ofelt, Force oscillateur, Durée vie radiative, Rapport branchement, Addition thulium, Borate, Monocristal, Matériau optique.
Wicri :
- topic : Dopage.

English descriptors

KwdEn :
- Absorption spectra, Borates, Branching ratio, Czochralski method, Doping, Judd-Ofelt theory, Monocrystals, Optical materials, Oscillator strengths, Radiative lifetimes, Specific heat, Thermal properties, Thulium additions.

Abstract

Single crystal of Tm³⁺: Li₆Gd (BO₃)₃ was grown by the Czochralski method. The heat capacity was measured from 308 to 673 K. The absorption spectra of the crystal in three mutually perpendicular arbitrary directions were measured at room temperature. Based on the Judd-Ofelt theory and the spectra measured in three mutually perpendicular directions, the intensity parameters Ω_t (t = 2, 4, 6), the line strengths, the oscillator strengths, the radiative rates, radiative lifetimes and fluorescent branching ratios were calculated. We calculated the emission cross-section by the reciprocity method and also obtained the gain cross-section.

A01	`01`	`1`		`@0 0022-2313`
A02	`01`			`@0 JLUMA8`
A03		`1`		`@0 J. lumin.`
A05				`@2 128`
A06				`@2 10`
A08	`01`	`1`	`ENG`	`@1 Thermal and optical properties of Tm³⁺: Li₆Gd(BO₃)₃ crystal : A potential candidate for 1.83 μm lasers`
A11	`01`	`1`		`@1 XINGHUA MA`
A11	`02`	`1`		`@1 JIANFU LI`
A11	`03`	`1`		`@1 ZHAOJIE ZHU`
A11	`04`	`1`		`@1 ZHENYU YOU`
A11	`05`	`1`		`@1 YAN WANG`
A11	`06`	`1`		`@1 CHAOYANG TU`
A14	`01`			`@1 Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155 @2 Fuzhou, Fujian 350002 @3 CHN @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut.`
A14	`02`			`@1 Graduate School of Chinese Academy of Sciences @2 Beijing 100039 @3 CHN @Z 1 aut.`
A20				`@1 1660-1664`
A21				`@1 2008`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 14666 @5 354000196485430180`
A44				`@0 0000 @1 © 2008 INIST-CNRS. All rights reserved.`
A45				`@0 28 ref.`
A47	`01`	`1`		`@0 08-0399143`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of luminescence`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 Single crystal of Tm³⁺: Li₆Gd (BO₃)₃ was grown by the Czochralski method. The heat capacity was measured from 308 to 673 K. The absorption spectra of the crystal in three mutually perpendicular arbitrary directions were measured at room temperature. Based on the Judd-Ofelt theory and the spectra measured in three mutually perpendicular directions, the intensity parameters Ω_t (t = 2, 4, 6), the line strengths, the oscillator strengths, the radiative rates, radiative lifetimes and fluorescent branching ratios were calculated. We calculated the emission cross-section by the reciprocity method and also obtained the gain cross-section.
C02	`01`	`3`		`@0 001B70H20`
C03	`01`	`3`	`FRE`	`@0 Propriété thermique @5 02`
C03	`01`	`3`	`ENG`	`@0 Thermal properties @5 02`
C03	`02`	`X`	`FRE`	`@0 Dopage @5 03`
C03	`02`	`X`	`ENG`	`@0 Doping @5 03`
C03	`02`	`X`	`SPA`	`@0 Doping @5 03`
C03	`03`	`3`	`FRE`	`@0 Méthode Czochralski @5 04`
C03	`03`	`3`	`ENG`	`@0 Czochralski method @5 04`
C03	`04`	`3`	`FRE`	`@0 Chaleur massique @5 05`
C03	`04`	`3`	`ENG`	`@0 Specific heat @5 05`
C03	`05`	`3`	`FRE`	`@0 Spectre absorption @5 06`
C03	`05`	`3`	`ENG`	`@0 Absorption spectra @5 06`
C03	`06`	`3`	`FRE`	`@0 Théorie Judd Ofelt @5 07`
C03	`06`	`3`	`ENG`	`@0 Judd-Ofelt theory @5 07`
C03	`07`	`3`	`FRE`	`@0 Force oscillateur @5 08`
C03	`07`	`3`	`ENG`	`@0 Oscillator strengths @5 08`
C03	`08`	`3`	`FRE`	`@0 Durée vie radiative @5 09`
C03	`08`	`3`	`ENG`	`@0 Radiative lifetimes @5 09`
C03	`09`	`3`	`FRE`	`@0 Rapport branchement @5 10`
C03	`09`	`3`	`ENG`	`@0 Branching ratio @5 10`
C03	`10`	`3`	`FRE`	`@0 Addition thulium @5 11`
C03	`10`	`3`	`ENG`	`@0 Thulium additions @5 11`
C03	`11`	`3`	`FRE`	`@0 Borate @2 NA @5 15`
C03	`11`	`3`	`ENG`	`@0 Borates @2 NA @5 15`
C03	`12`	`3`	`FRE`	`@0 Monocristal @5 16`
C03	`12`	`3`	`ENG`	`@0 Monocrystals @5 16`
C03	`13`	`3`	`FRE`	`@0 Matériau optique @5 17`
C03	`13`	`3`	`ENG`	`@0 Optical materials @5 17`
N21				`@1 259`

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Pascal:08-0399143

Le document en format XML

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: Li<sub>6</sub>
Gd(BO<sub>3</sub>
)<sub>3</sub>
 crystal : A potential candidate for 1.83 μm lasers</title>
<author><name sortKey="Xinghua Ma" sort="Xinghua Ma" uniqKey="Xinghua Ma" last="Xinghua Ma">XINGHUA MA</name>
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<s2>Fuzhou, Fujian 350002</s2>
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<author><name sortKey="Zhenyu You" sort="Zhenyu You" uniqKey="Zhenyu You" last="Zhenyu You">ZHENYU YOU</name>
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<s2>Fuzhou, Fujian 350002</s2>
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<author><name sortKey="Yan Wang" sort="Yan Wang" uniqKey="Yan Wang" last="Yan Wang">YAN WANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</s2>
<s3>CHN</s3>
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<country>République populaire de Chine</country>
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<author><name sortKey="Chaoyang Tu" sort="Chaoyang Tu" uniqKey="Chaoyang Tu" last="Chaoyang Tu">CHAOYANG TU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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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<idno type="RBID">Pascal:08-0399143</idno>
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<idno type="wicri:Area/Pascal/Curation">000617</idno>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Thermal and optical properties of Tm<sup>3+</sup>
: Li<sub>6</sub>
Gd(BO<sub>3</sub>
)<sub>3</sub>
 crystal : A potential candidate for 1.83 μm lasers</title>
<author><name sortKey="Xinghua Ma" sort="Xinghua Ma" uniqKey="Xinghua Ma" last="Xinghua Ma">XINGHUA MA</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
</inist:fA14>
<country>République populaire de Chine</country>
</affiliation>
</author>
<author><name sortKey="Jianfu Li" sort="Jianfu Li" uniqKey="Jianfu Li" last="Jianfu Li">JIANFU LI</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
<author><name sortKey="Zhaojie Zhu" sort="Zhaojie Zhu" uniqKey="Zhaojie Zhu" last="Zhaojie Zhu">ZHAOJIE ZHU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
<author><name sortKey="Zhenyu You" sort="Zhenyu You" uniqKey="Zhenyu You" last="Zhenyu You">ZHENYU YOU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
<author><name sortKey="Yan Wang" sort="Yan Wang" uniqKey="Yan Wang" last="Yan Wang">YAN WANG</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
<author><name sortKey="Chaoyang Tu" sort="Chaoyang Tu" uniqKey="Chaoyang Tu" last="Chaoyang Tu">CHAOYANG TU</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
</analytic>
<series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
<imprint><date when="2008">2008</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Absorption spectra</term>
<term>Borates</term>
<term>Branching ratio</term>
<term>Czochralski method</term>
<term>Doping</term>
<term>Judd-Ofelt theory</term>
<term>Monocrystals</term>
<term>Optical materials</term>
<term>Oscillator strengths</term>
<term>Radiative lifetimes</term>
<term>Specific heat</term>
<term>Thermal properties</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Propriété thermique</term>
<term>Dopage</term>
<term>Méthode Czochralski</term>
<term>Chaleur massique</term>
<term>Spectre absorption</term>
<term>Théorie Judd Ofelt</term>
<term>Force oscillateur</term>
<term>Durée vie radiative</term>
<term>Rapport branchement</term>
<term>Addition thulium</term>
<term>Borate</term>
<term>Monocristal</term>
<term>Matériau optique</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Dopage</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Single crystal of Tm<sup>3+</sup>
: Li<sub>6</sub>
Gd (BO<sub>3</sub>
)<sub>3</sub>
 was grown by the Czochralski method. The heat capacity was measured from 308 to 673 K. The absorption spectra of the crystal in three mutually perpendicular arbitrary directions were measured at room temperature. Based on the Judd-Ofelt theory and the spectra measured in three mutually perpendicular directions, the intensity parameters Ω<sub>t</sub>
 (t = 2, 4, 6), the line strengths, the oscillator strengths, the radiative rates, radiative lifetimes and fluorescent branching ratios were calculated. We calculated the emission cross-section by the reciprocity method and also obtained the gain cross-section.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-2313</s0>
</fA01>
<fA02 i1="01"><s0>JLUMA8</s0>
</fA02>
<fA03 i2="1"><s0>J. lumin.</s0>
</fA03>
<fA05><s2>128</s2>
</fA05>
<fA06><s2>10</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Thermal and optical properties of Tm<sup>3+</sup>
: Li<sub>6</sub>
Gd(BO<sub>3</sub>
)<sub>3</sub>
 crystal : A potential candidate for 1.83 μm lasers</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>XINGHUA MA</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>JIANFU LI</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>ZHAOJIE ZHU</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>ZHENYU YOU</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>YAN WANG</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>CHAOYANG TU</s1>
</fA11>
<fA14 i1="01"><s1>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155</s1>
<s2>Fuzhou, Fujian 350002</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>
</fA14>
<fA20><s1>1660-1664</s1>
</fA20>
<fA21><s1>2008</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>14666</s2>
<s5>354000196485430180</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2008 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>28 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>08-0399143</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Journal of luminescence</s0>
</fA64>
<fA66 i1="01"><s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Single crystal of Tm<sup>3+</sup>
: Li<sub>6</sub>
Gd (BO<sub>3</sub>
)<sub>3</sub>
 was grown by the Czochralski method. The heat capacity was measured from 308 to 673 K. The absorption spectra of the crystal in three mutually perpendicular arbitrary directions were measured at room temperature. Based on the Judd-Ofelt theory and the spectra measured in three mutually perpendicular directions, the intensity parameters Ω<sub>t</sub>
 (t = 2, 4, 6), the line strengths, the oscillator strengths, the radiative rates, radiative lifetimes and fluorescent branching ratios were calculated. We calculated the emission cross-section by the reciprocity method and also obtained the gain cross-section.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70H20</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Propriété thermique</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Thermal properties</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Dopage</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Doping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Doping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Méthode Czochralski</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Czochralski method</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Chaleur massique</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Specific heat</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Spectre absorption</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Absorption spectra</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Théorie Judd Ofelt</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Judd-Ofelt theory</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Force oscillateur</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Oscillator strengths</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Durée vie radiative</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Radiative lifetimes</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Rapport branchement</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Branching ratio</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Borate</s0>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Borates</s0>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Monocristal</s0>
<s5>16</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Monocrystals</s0>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Matériau optique</s0>
<s5>17</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Optical materials</s0>
<s5>17</s5>
</fC03>
<fN21><s1>259</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers

Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers

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