ThuliumV1, Pascal, Curation, bibRecord, 000533

Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO3

Identifieur interne : 000533 ( Pascal/Curation ); précédent : 000532; suivant : 000534

Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO3

Auteurs : B. Q. Yao [République populaire de Chine] ; L. L. Zheng [République populaire de Chine] ; R. L. Zhou [République populaire de Chine] ; X. M. Duan [République populaire de Chine] ; Y. J. Zhang [République populaire de Chine] ; Y. L. Ju [République populaire de Chine] ; Y. Z. Wang [République populaire de Chine] ; G. J. Zhao [République populaire de Chine] ; Q. Dong [République populaire de Chine]

Source :

Laser physics [ 1054-660X ] ; 2008.

RBID : Pascal:09-0127514

Descripteurs français

Pascal (Inist)
- Pompage par extrémité, Pompage par laser, Laser continu, Laser solide, Température ambiante, Polarisation rectiligne, Composé ternaire, Matériau dopé, Addition holmium, Puissance sortie, YAlO3, Al O Y, 4260P, 4255R.

English descriptors

KwdEn :
- Ambient temperature, CW lasers, Doped materials, End pumping, Holmium additions, Laser pumping, Linear polarization, Output power, Solid state lasers, Ternary compounds.

Abstract

-We report on the room-temperature continuous-wave (CW) operation of a Ho:YAlO₃ laser that is resonantly end pumped at 1.94 μm by a diode-pumped thulium-doped laser in the same host. Through the use of a 1 at % Ho³⁺-doped 20-mm-long YAlO₃ crystal (b cut), the Ho:YAlO₃ laser generated 1 W of linearly polarized (Ellc) output at 2118 nm and 0.55 W of Ella output at 2128.5 nm for an incident pump power of 5 W, with an output coupler transmission of 14 and 3%, respectively. An optical-to-optical conversion efficiency of 20% and a slope efficiency of 33% were achieved at 2118 nm corresponding to an incident pump power.

A01	`01`	`1`		`@0 1054-660X`
A03		`1`		`@0 Laser phys.`
A05				`@2 18`
A06				`@2 12`
A08	`01`	`1`	`ENG`	`@1 Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO₃`
A11	`01`	`1`		`@1 YAO (B. Q.)`
A11	`02`	`1`		`@1 ZHENG (L. L.)`
A11	`03`	`1`		`@1 ZHOU (R. L.)`
A11	`04`	`1`		`@1 DUAN (X. M.)`
A11	`05`	`1`		`@1 ZHANG (Y. J.)`
A11	`06`	`1`		`@1 JU (Y. L.)`
A11	`07`	`1`		`@1 WANG (Y. Z.)`
A11	`08`	`1`		`@1 ZHAO (G. J.)`
A11	`09`	`1`		`@1 DONG (Q.)`
A14	`01`			`@1 National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology @2 Harbin, 150001 @3 CHN @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut. @Z 9 aut.`
A14	`02`			`@1 R&D Center for Laser and Opto-Electronic Materials, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences @2 Shanghai, 201800 @3 CHN @Z 8 aut.`
A20				`@1 1501-1504`
A21				`@1 2008`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 26554 @5 354000184170800160`
A44				`@0 0000 @1 © 2009 INIST-CNRS. All rights reserved.`
A45				`@0 15 ref.`
A47	`01`	`1`		`@0 09-0127514`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Laser physics`
A66	`01`			`@0 USA`
C01	`01`		`ENG`	@0 -We report on the room-temperature continuous-wave (CW) operation of a Ho:YAlO₃ laser that is resonantly end pumped at 1.94 μm by a diode-pumped thulium-doped laser in the same host. Through the use of a 1 at % Ho³⁺-doped 20-mm-long YAlO₃ crystal (b cut), the Ho:YAlO₃ laser generated 1 W of linearly polarized (Ellc) output at 2118 nm and 0.55 W of Ella output at 2128.5 nm for an incident pump power of 5 W, with an output coupler transmission of 14 and 3%, respectively. An optical-to-optical conversion efficiency of 20% and a slope efficiency of 33% were achieved at 2118 nm corresponding to an incident pump power.
C02	`01`	`3`		`@0 001B40B55R`
C02	`02`	`3`		`@0 001B40B60P`
C03	`01`	`3`	`FRE`	`@0 Pompage par extrémité @5 03`
C03	`01`	`3`	`ENG`	`@0 End pumping @5 03`
C03	`02`	`3`	`FRE`	`@0 Pompage par laser @5 05`
C03	`02`	`3`	`ENG`	`@0 Laser pumping @5 05`
C03	`03`	`3`	`FRE`	`@0 Laser continu @5 11`
C03	`03`	`3`	`ENG`	`@0 CW lasers @5 11`
C03	`04`	`3`	`FRE`	`@0 Laser solide @5 12`
C03	`04`	`3`	`ENG`	`@0 Solid state lasers @5 12`
C03	`05`	`3`	`FRE`	`@0 Température ambiante @5 41`
C03	`05`	`3`	`ENG`	`@0 Ambient temperature @5 41`
C03	`06`	`3`	`FRE`	`@0 Polarisation rectiligne @5 42`
C03	`06`	`3`	`ENG`	`@0 Linear polarization @5 42`
C03	`07`	`3`	`FRE`	`@0 Composé ternaire @5 50`
C03	`07`	`3`	`ENG`	`@0 Ternary compounds @5 50`
C03	`08`	`3`	`FRE`	`@0 Matériau dopé @5 51`
C03	`08`	`3`	`ENG`	`@0 Doped materials @5 51`
C03	`09`	`3`	`FRE`	`@0 Addition holmium @5 57`
C03	`09`	`3`	`ENG`	`@0 Holmium additions @5 57`
C03	`10`	`X`	`FRE`	`@0 Puissance sortie @5 61`
C03	`10`	`X`	`ENG`	`@0 Output power @5 61`
C03	`10`	`X`	`SPA`	`@0 Potencia salida @5 61`
C03	`11`	`3`	`FRE`	`@0 YAlO3 @4 INC @5 71`
C03	`12`	`3`	`FRE`	`@0 Al O Y @4 INC @5 75`
C03	`13`	`3`	`FRE`	`@0 4260P @4 INC @5 83`
C03	`14`	`3`	`FRE`	`@0 4255R @4 INC @5 84`
N21				`@1 089`

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Pascal:09-0127514

Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO<sub>3</sub>
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<author><name sortKey="Yao, B Q" sort="Yao, B Q" uniqKey="Yao B" first="B. Q." last="Yao">B. Q. Yao</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology</s1>
<s2>Harbin, 150001</s2>
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<s2>Harbin, 150001</s2>
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<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology</s1>
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<s2>Shanghai, 201800</s2>
<s3>CHN</s3>
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<author><name sortKey="Dong, Q" sort="Dong, Q" uniqKey="Dong Q" first="Q." last="Dong">Q. Dong</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology</s1>
<s2>Harbin, 150001</s2>
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</analytic>
<series><title level="j" type="main">Laser physics</title>
<title level="j" type="abbreviated">Laser phys.</title>
<idno type="ISSN">1054-660X</idno>
<imprint><date when="2008">2008</date>
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<idno type="ISSN">1054-660X</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Ambient temperature</term>
<term>CW lasers</term>
<term>Doped materials</term>
<term>End pumping</term>
<term>Holmium additions</term>
<term>Laser pumping</term>
<term>Linear polarization</term>
<term>Output power</term>
<term>Solid state lasers</term>
<term>Ternary compounds</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Pompage par extrémité</term>
<term>Pompage par laser</term>
<term>Laser continu</term>
<term>Laser solide</term>
<term>Température ambiante</term>
<term>Polarisation rectiligne</term>
<term>Composé ternaire</term>
<term>Matériau dopé</term>
<term>Addition holmium</term>
<term>Puissance sortie</term>
<term>YAlO3</term>
<term>Al O Y</term>
<term>4260P</term>
<term>4255R</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">-We report on the room-temperature continuous-wave (CW) operation of a Ho:YAlO<sub>3</sub>
 laser that is resonantly end pumped at 1.94 μm by a diode-pumped thulium-doped laser in the same host. Through the use of a 1 at % Ho<sup>3+</sup>
-doped 20-mm-long YAlO<sub>3</sub>
 crystal (b cut), the Ho:YAlO<sub>3</sub>
 laser generated 1 W of linearly polarized (Ellc) output at 2118 nm and 0.55 W of Ella output at 2128.5 nm for an incident pump power of 5 W, with an output coupler transmission of 14 and 3%, respectively. An optical-to-optical conversion efficiency of 20% and a slope efficiency of 33% were achieved at 2118 nm corresponding to an incident pump power.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1054-660X</s0>
</fA01>
<fA03 i2="1"><s0>Laser phys.</s0>
</fA03>
<fA05><s2>18</s2>
</fA05>
<fA06><s2>12</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO<sub>3</sub>
</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>YAO (B. Q.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>ZHENG (L. L.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>ZHOU (R. L.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>DUAN (X. M.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>ZHANG (Y. J.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>JU (Y. L.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>WANG (Y. Z.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>ZHAO (G. J.)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>DONG (Q.)</s1>
</fA11>
<fA14 i1="01"><s1>National Key Laboratory of Tunable Laser Technology, Harbin Institute of Technology</s1>
<s2>Harbin, 150001</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>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>R&D Center for Laser and Opto-Electronic Materials, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences</s1>
<s2>Shanghai, 201800</s2>
<s3>CHN</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA20><s1>1501-1504</s1>
</fA20>
<fA21><s1>2008</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>26554</s2>
<s5>354000184170800160</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2009 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>15 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>09-0127514</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Laser physics</s0>
</fA64>
<fA66 i1="01"><s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>-We report on the room-temperature continuous-wave (CW) operation of a Ho:YAlO<sub>3</sub>
 laser that is resonantly end pumped at 1.94 μm by a diode-pumped thulium-doped laser in the same host. Through the use of a 1 at % Ho<sup>3+</sup>
-doped 20-mm-long YAlO<sub>3</sub>
 crystal (b cut), the Ho:YAlO<sub>3</sub>
 laser generated 1 W of linearly polarized (Ellc) output at 2118 nm and 0.55 W of Ella output at 2128.5 nm for an incident pump power of 5 W, with an output coupler transmission of 14 and 3%, respectively. An optical-to-optical conversion efficiency of 20% and a slope efficiency of 33% were achieved at 2118 nm corresponding to an incident pump power.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B55R</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B40B60P</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Pompage par extrémité</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>End pumping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Pompage par laser</s0>
<s5>05</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Laser pumping</s0>
<s5>05</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Laser continu</s0>
<s5>11</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>CW lasers</s0>
<s5>11</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Laser solide</s0>
<s5>12</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Solid state lasers</s0>
<s5>12</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Température ambiante</s0>
<s5>41</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Ambient temperature</s0>
<s5>41</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Polarisation rectiligne</s0>
<s5>42</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Linear polarization</s0>
<s5>42</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Composé ternaire</s0>
<s5>50</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Ternary compounds</s0>
<s5>50</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>51</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>51</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Addition holmium</s0>
<s5>57</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Holmium additions</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Puissance sortie</s0>
<s5>61</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Output power</s0>
<s5>61</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Potencia salida</s0>
<s5>61</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>YAlO3</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Al O Y</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>4260P</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>4255R</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fN21><s1>089</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO3

Holmium Laser In-Band Pumped by a Thulium Laser in the Same Host of YAlO3

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