ThuliumV1, Pascal, Corpus, bibRecord, 000496

High repetition rate, high peak power, diode pumped Tm:YLF laser

Identifieur interne : 000496 ( Pascal/Corpus ); précédent : 000495; suivant : 000497

High repetition rate, high peak power, diode pumped Tm:YLF laser

Auteurs : J. K. Jabczynski ; L. Gorajek ; W. Zendzian ; J. Kwiatkowski ; H. Jelinkova ; J. Sulc ; M. Nemec

Source :

Laser physics letters : (Print) [ 1612-2011 ] ; 2009.

RBID : Pascal:09-0248187

Descripteurs français

Pascal (Inist)
- Pompage par diode, Laser semiconducteur, Résonateur cavité, Modulateur acoustooptique, Laser déclenché, Laser solide, Taux répétition élevé, Température ambiante, Puissance sortie, Domaine temps ns, Durée impulsion, Matériau dopé, Addition thulium, Yttrium Fluorure, Lithium Fluorure, Silice fusionnée, Laser YLF, 4255X, 4260G, 4255R.

English descriptors

KwdEn :
- Acoustooptical modulator, Ambient temperature, Cavity resonators, Diode pumping, Doped materials, High repetition rate, Lithium Fluorides, Output power, Pulse width, Q switched laser, Semiconductor lasers, Solid state lasers, Thulium additions, Yttrium Fluorides, ns range.

Abstract

The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2_-plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 1612-2011`
A03		`1`		`@0 Laser phys. lett. : (Print)`
A05				`@2 6`
A06				`@2 2`
A08	`01`	`1`	`ENG`	`@1 High repetition rate, high peak power, diode pumped Tm:YLF laser`
A11	`01`	`1`		`@1 JABCZYNSKI (J. K.)`
A11	`02`	`1`		`@1 GORAJEK (L.)`
A11	`03`	`1`		`@1 ZENDZIAN (W.)`
A11	`04`	`1`		`@1 KWIATKOWSKI (J.)`
A11	`05`	`1`		`@1 JELINKOVA (H.)`
A11	`06`	`1`		`@1 SULC (J.)`
A11	`07`	`1`		`@1 NEMEC (M.)`
A14	`01`			`@1 Institute of Optoelectronics, Military University of Technology, ul. gen. S. Kaliskiego 2 @2 00-908 Warsaw @3 POL @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut.`
A14	`02`			`@1 Czech Technical University, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7 @2 115 19 Prague @3 CZE @Z 5 aut. @Z 6 aut. @Z 7 aut.`
A20				`@1 109-112`
A21				`@1 2009`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 28000 @5 354000186216160050`
A44				`@0 0000 @1 © 2009 INIST-CNRS. All rights reserved.`
A45				`@0 23 ref.`
A47	`01`	`1`		`@0 09-0248187`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Laser physics letters : (Print)`
A66	`01`			`@0 DEU`
C01	`01`		`ENG`	@0 The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2_-plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.
C02	`01`	`3`		`@0 001B40B55X`
C02	`02`	`3`		`@0 001B40B55P`
C02	`03`	`3`		`@0 001B40B60G`
C02	`04`	`3`		`@0 001B40B55R`
C03	`01`	`X`	`FRE`	`@0 Pompage par diode @5 03`
C03	`01`	`X`	`ENG`	`@0 Diode pumping @5 03`
C03	`01`	`X`	`SPA`	`@0 Bombeo por diodo @5 03`
C03	`02`	`3`	`FRE`	`@0 Laser semiconducteur @5 09`
C03	`02`	`3`	`ENG`	`@0 Semiconductor lasers @5 09`
C03	`03`	`3`	`FRE`	`@0 Résonateur cavité @5 12`
C03	`03`	`3`	`ENG`	`@0 Cavity resonators @5 12`
C03	`04`	`X`	`FRE`	`@0 Modulateur acoustooptique @5 13`
C03	`04`	`X`	`ENG`	`@0 Acoustooptical modulator @5 13`
C03	`04`	`X`	`SPA`	`@0 Modulador acústico-óptico @5 13`
C03	`05`	`X`	`FRE`	`@0 Laser déclenché @5 14`
C03	`05`	`X`	`ENG`	`@0 Q switched laser @5 14`
C03	`05`	`X`	`SPA`	`@0 Laser disparado @5 14`
C03	`06`	`3`	`FRE`	`@0 Laser solide @5 15`
C03	`06`	`3`	`ENG`	`@0 Solid state lasers @5 15`
C03	`07`	`3`	`FRE`	`@0 Taux répétition élevé @5 41`
C03	`07`	`3`	`ENG`	`@0 High repetition rate @5 41`
C03	`08`	`3`	`FRE`	`@0 Température ambiante @5 42`
C03	`08`	`3`	`ENG`	`@0 Ambient temperature @5 42`
C03	`09`	`X`	`FRE`	`@0 Puissance sortie @5 43`
C03	`09`	`X`	`ENG`	`@0 Output power @5 43`
C03	`09`	`X`	`SPA`	`@0 Potencia salida @5 43`
C03	`10`	`3`	`FRE`	`@0 Domaine temps ns @5 44`
C03	`10`	`3`	`ENG`	`@0 ns range @5 44`
C03	`11`	`X`	`FRE`	`@0 Durée impulsion @5 45`
C03	`11`	`X`	`ENG`	`@0 Pulse width @5 45`
C03	`11`	`X`	`SPA`	`@0 Duración impulso @5 45`
C03	`12`	`3`	`FRE`	`@0 Matériau dopé @5 50`
C03	`12`	`3`	`ENG`	`@0 Doped materials @5 50`
C03	`13`	`3`	`FRE`	`@0 Addition thulium @5 61`
C03	`13`	`3`	`ENG`	`@0 Thulium additions @5 61`
C03	`14`	`3`	`FRE`	`@0 Yttrium Fluorure @2 NC @2 NA @5 62`
C03	`14`	`3`	`ENG`	`@0 Yttrium Fluorides @2 NC @2 NA @5 62`
C03	`15`	`3`	`FRE`	`@0 Lithium Fluorure @2 NC @2 NA @5 63`
C03	`15`	`3`	`ENG`	`@0 Lithium Fluorides @2 NC @2 NA @5 63`
C03	`16`	`3`	`FRE`	`@0 Silice fusionnée @4 INC @5 71`
C03	`17`	`3`	`FRE`	`@0 Laser YLF @4 INC @5 83`
C03	`18`	`3`	`FRE`	`@0 4255X @4 INC @5 91`
C03	`19`	`3`	`FRE`	`@0 4260G @4 INC @5 93`
C03	`20`	`3`	`FRE`	`@0 4255R @4 INC @5 94`
N21				`@1 187`

Format Inist (serveur)

NO :	PASCAL 09-0248187 INIST
ET :	High repetition rate, high peak power, diode pumped Tm:YLF laser
AU :	JABCZYNSKI (J. K.); GORAJEK (L.); ZENDZIAN (W.); KWIATKOWSKI (J.); JELINKOVA (H.); SULC (J.); NEMEC (M.)
AF :	Institute of Optoelectronics, Military University of Technology, ul. gen. S. Kaliskiego 2/00-908 Warsaw/Pologne (1 aut., 2 aut., 3 aut., 4 aut.); Czech Technical University, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7/115 19 Prague/Tchèque, République (5 aut., 6 aut., 7 aut.)
DT :	Publication en série; Niveau analytique
SO :	Laser physics letters : (Print); ISSN 1612-2011; Allemagne; Da. 2009; Vol. 6; No. 2; Pp. 109-112; Bibl. 23 ref.
LA :	Anglais
EA :	The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2_-plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.
CC :	001B40B55X; 001B40B55P; 001B40B60G; 001B40B55R
FD :	Pompage par diode; Laser semiconducteur; Résonateur cavité; Modulateur acoustooptique; Laser déclenché; Laser solide; Taux répétition élevé; Température ambiante; Puissance sortie; Domaine temps ns; Durée impulsion; Matériau dopé; Addition thulium; Yttrium Fluorure; Lithium Fluorure; Silice fusionnée; Laser YLF; 4255X; 4260G; 4255R
ED :	Diode pumping; Semiconductor lasers; Cavity resonators; Acoustooptical modulator; Q switched laser; Solid state lasers; High repetition rate; Ambient temperature; Output power; ns range; Pulse width; Doped materials; Thulium additions; Yttrium Fluorides; Lithium Fluorides
SD :	Bombeo por diodo; Modulador acústico-óptico; Laser disparado; Potencia salida; Duración impulso
LO :	INIST-28000.354000186216160050
ID :	09-0248187

Links to Exploration step

Pascal:09-0248187

Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">High repetition rate, high peak power, diode pumped Tm:YLF laser</title>
<author><name sortKey="Jabczynski, J K" sort="Jabczynski, J K" uniqKey="Jabczynski J" first="J. K." last="Jabczynski">J. K. Jabczynski</name>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
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<author><name sortKey="Gorajek, L" sort="Gorajek, L" uniqKey="Gorajek L" first="L." last="Gorajek">L. Gorajek</name>
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<sZ>3 aut.</sZ>
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</author>
<author><name sortKey="Kwiatkowski, J" sort="Kwiatkowski, J" uniqKey="Kwiatkowski J" first="J." last="Kwiatkowski">J. Kwiatkowski</name>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
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<sZ>6 aut.</sZ>
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<series><title level="j" type="main">Laser physics letters : (Print)</title>
<title level="j" type="abbreviated">Laser phys. lett. : (Print)</title>
<idno type="ISSN">1612-2011</idno>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Acoustooptical modulator</term>
<term>Ambient temperature</term>
<term>Cavity resonators</term>
<term>Diode pumping</term>
<term>Doped materials</term>
<term>High repetition rate</term>
<term>Lithium Fluorides</term>
<term>Output power</term>
<term>Pulse width</term>
<term>Q switched laser</term>
<term>Semiconductor lasers</term>
<term>Solid state lasers</term>
<term>Thulium additions</term>
<term>Yttrium Fluorides</term>
<term>ns range</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Pompage par diode</term>
<term>Laser semiconducteur</term>
<term>Résonateur cavité</term>
<term>Modulateur acoustooptique</term>
<term>Laser déclenché</term>
<term>Laser solide</term>
<term>Taux répétition élevé</term>
<term>Température ambiante</term>
<term>Puissance sortie</term>
<term>Domaine temps ns</term>
<term>Durée impulsion</term>
<term>Matériau dopé</term>
<term>Addition thulium</term>
<term>Yttrium Fluorure</term>
<term>Lithium Fluorure</term>
<term>Silice fusionnée</term>
<term>Laser YLF</term>
<term>4255X</term>
<term>4260G</term>
<term>4255R</term>
</keywords>
</textClass>
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</teiHeader>
<front><div type="abstract" xml:lang="en">The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2<sub>-</sub>
plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1612-2011</s0>
</fA01>
<fA03 i2="1"><s0>Laser phys. lett. : (Print)</s0>
</fA03>
<fA05><s2>6</s2>
</fA05>
<fA06><s2>2</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>High repetition rate, high peak power, diode pumped Tm:YLF laser</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>JABCZYNSKI (J. K.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>GORAJEK (L.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>ZENDZIAN (W.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>KWIATKOWSKI (J.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>JELINKOVA (H.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>SULC (J.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>NEMEC (M.)</s1>
</fA11>
<fA14 i1="01"><s1>Institute of Optoelectronics, Military University of Technology, ul. gen. S. Kaliskiego 2</s1>
<s2>00-908 Warsaw</s2>
<s3>POL</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Czech Technical University, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7</s1>
<s2>115 19 Prague</s2>
<s3>CZE</s3>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</fA14>
<fA20><s1>109-112</s1>
</fA20>
<fA21><s1>2009</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>28000</s2>
<s5>354000186216160050</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2009 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>23 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>09-0248187</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Laser physics letters : (Print)</s0>
</fA64>
<fA66 i1="01"><s0>DEU</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2<sub>-</sub>
plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B55X</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B40B55P</s0>
</fC02>
<fC02 i1="03" i2="3"><s0>001B40B60G</s0>
</fC02>
<fC02 i1="04" i2="3"><s0>001B40B55R</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Pompage par diode</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Diode pumping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Bombeo por diodo</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Laser semiconducteur</s0>
<s5>09</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Semiconductor lasers</s0>
<s5>09</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Résonateur cavité</s0>
<s5>12</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Cavity resonators</s0>
<s5>12</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Modulateur acoustooptique</s0>
<s5>13</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Acoustooptical modulator</s0>
<s5>13</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Modulador acústico-óptico</s0>
<s5>13</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Laser déclenché</s0>
<s5>14</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Q switched laser</s0>
<s5>14</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Laser disparado</s0>
<s5>14</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Laser solide</s0>
<s5>15</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Solid state lasers</s0>
<s5>15</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Taux répétition élevé</s0>
<s5>41</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>High repetition rate</s0>
<s5>41</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Température ambiante</s0>
<s5>42</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Ambient temperature</s0>
<s5>42</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Puissance sortie</s0>
<s5>43</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Output power</s0>
<s5>43</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Potencia salida</s0>
<s5>43</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Domaine temps ns</s0>
<s5>44</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>ns range</s0>
<s5>44</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Durée impulsion</s0>
<s5>45</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Pulse width</s0>
<s5>45</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Duración impulso</s0>
<s5>45</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>50</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>50</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>61</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>61</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Yttrium Fluorure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>62</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Yttrium Fluorides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>62</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Lithium Fluorure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>63</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Lithium Fluorides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>63</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Silice fusionnée</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Laser YLF</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>4255X</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>4260G</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>4255R</s0>
<s4>INC</s4>
<s5>94</s5>
</fC03>
<fN21><s1>187</s1>
</fN21>
</pA>
</standard>
<server><NO>PASCAL 09-0248187 INIST</NO>
<ET>High repetition rate, high peak power, diode pumped Tm:YLF laser</ET>
<AU>JABCZYNSKI (J. K.); GORAJEK (L.); ZENDZIAN (W.); KWIATKOWSKI (J.); JELINKOVA (H.); SULC (J.); NEMEC (M.)</AU>
<AF>Institute of Optoelectronics, Military University of Technology, ul. gen. S. Kaliskiego 2/00-908 Warsaw/Pologne (1 aut., 2 aut., 3 aut., 4 aut.); Czech Technical University, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7/115 19 Prague/Tchèque, République (5 aut., 6 aut., 7 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Laser physics letters : (Print); ISSN 1612-2011; Allemagne; Da. 2009; Vol. 6; No. 2; Pp. 109-112; Bibl. 23 ref.</SO>
<LA>Anglais</LA>
<EA>The room-temperature, water-cooled, diode pumped Tm:YLF laser head was elaborated and examined. For pumping the fiber coupled (0.2 mm core diameter) 25-W laser diode bar emitting at 792-nm wavelength was deployed. Near 5 W of CW output power and 25% slope efficiency was demonstrated in a short, 70-mm long resonator. Tuning in 1845-1935 nm wave-length range by means of 2<sub>-</sub>
plate Lyot filter was demonstrated only in free-running regime. The fused silica acousto-optic modulator with above 80% diffraction effieieney for 25-W power of RF was deployed as the Q-switch for such a laser. In the best case of Q-switching regime, up to 10-mJ output energy with 47-ns pulse duration, 220 kW peak power was demonstrated for 133 Hz. For higher repetition rate of 2 kHz, 12 kW peak power with 2.5 W of average power was achieved.</EA>
<CC>001B40B55X; 001B40B55P; 001B40B60G; 001B40B55R</CC>
<FD>Pompage par diode; Laser semiconducteur; Résonateur cavité; Modulateur acoustooptique; Laser déclenché; Laser solide; Taux répétition élevé; Température ambiante; Puissance sortie; Domaine temps ns; Durée impulsion; Matériau dopé; Addition thulium; Yttrium Fluorure; Lithium Fluorure; Silice fusionnée; Laser YLF; 4255X; 4260G; 4255R</FD>
<ED>Diode pumping; Semiconductor lasers; Cavity resonators; Acoustooptical modulator; Q switched laser; Solid state lasers; High repetition rate; Ambient temperature; Output power; ns range; Pulse width; Doped materials; Thulium additions; Yttrium Fluorides; Lithium Fluorides</ED>
<SD>Bombeo por diodo; Modulador acústico-óptico; Laser disparado; Potencia salida; Duración impulso</SD>
<LO>INIST-28000.354000186216160050</LO>
<ID>09-0248187</ID>
</server>
</inist>
</record>

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High repetition rate, high peak power, diode pumped Tm:YLF laser

High repetition rate, high peak power, diode pumped Tm:YLF laser

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