Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers
Identifieur interne : 000617 ( Pascal/Corpus ); précédent : 000616; suivant : 000618Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers
Auteurs : XINGHUA MA ; JIANFU LI ; ZHAOJIE ZHU ; ZHENYU YOU ; YAN WANG ; CHAOYANG TUSource :
- Journal of luminescence [ 0022-2313 ] ; 2008.
Descripteurs français
- Pascal (Inist)
English descriptors
- KwdEn :
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 Ωt (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.
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Pour connaître la documentation sur le format Inist Standard.
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Format Inist (serveur)
NO : | PASCAL 08-0399143 INIST |
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ET : | Thermal and optical properties of Tm3+: Li6Gd(BO3)3 crystal : A potential candidate for 1.83 μm lasers |
AU : | XINGHUA MA; JIANFU LI; ZHAOJIE ZHU; ZHENYU YOU; YAN WANG; CHAOYANG TU |
AF : | Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155/Fuzhou, Fujian 350002/Chine (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 6 aut.); Graduate School of Chinese Academy of Sciences/Beijing 100039/Chine (1 aut.) |
DT : | Publication en série; Niveau analytique |
SO : | Journal of luminescence; ISSN 0022-2313; Coden JLUMA8; Pays-Bas; Da. 2008; Vol. 128; No. 10; Pp. 1660-1664; Bibl. 28 ref. |
LA : | Anglais |
EA : | 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 Ωt (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. |
CC : | 001B70H20 |
FD : | 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 |
ED : | Thermal properties; Doping; Czochralski method; Specific heat; Absorption spectra; Judd-Ofelt theory; Oscillator strengths; Radiative lifetimes; Branching ratio; Thulium additions; Borates; Monocrystals; Optical materials |
SD : | Doping |
LO : | INIST-14666.354000196485430180 |
ID : | 08-0399143 |
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Pascal:08-0399143Le 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>
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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><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>
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<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
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<affiliation><inist:fA14 i1="02"><s1>Graduate School of Chinese Academy of Sciences</s1>
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<author><name sortKey="Jianfu Li" sort="Jianfu Li" uniqKey="Jianfu Li" last="Jianfu Li">JIANFU LI</name>
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<affiliation><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>
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<author><name sortKey="Chaoyang Tu" sort="Chaoyang Tu" uniqKey="Chaoyang Tu" last="Chaoyang Tu">CHAOYANG TU</name>
<affiliation><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>
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<series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
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<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>
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<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>
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<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>
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<fA20><s1>1660-1664</s1>
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<fA45><s0>28 ref.</s0>
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<fA47 i1="01" i2="1"><s0>08-0399143</s0>
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<fA60><s1>P</s1>
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<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>
<server><NO>PASCAL 08-0399143 INIST</NO>
<ET>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</ET>
<AU>XINGHUA MA; JIANFU LI; ZHAOJIE ZHU; ZHENYU YOU; YAN WANG; CHAOYANG TU</AU>
<AF>Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences, Key Laboratory of Materials Chemistry and Physics, Yangqiao West Road 155/Fuzhou, Fujian 350002/Chine (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 6 aut.); Graduate School of Chinese Academy of Sciences/Beijing 100039/Chine (1 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Journal of luminescence; ISSN 0022-2313; Coden JLUMA8; Pays-Bas; Da. 2008; Vol. 128; No. 10; Pp. 1660-1664; Bibl. 28 ref.</SO>
<LA>Anglais</LA>
<EA>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.</EA>
<CC>001B70H20</CC>
<FD>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</FD>
<ED>Thermal properties; Doping; Czochralski method; Specific heat; Absorption spectra; Judd-Ofelt theory; Oscillator strengths; Radiative lifetimes; Branching ratio; Thulium additions; Borates; Monocrystals; Optical materials</ED>
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