ThuliumV1, Pascal, Curation, bibRecord, 001889

Investigation of 2.1-μm lasing properties of Ho:Tm:Cr:YAG crystals under flash-lamp pumping at various operating conditions

Identifieur interne : 001889 ( Pascal/Curation ); précédent : 001888; suivant : 001890

Investigation of 2.1-μm lasing properties of Ho:Tm:Cr:YAG crystals under flash-lamp pumping at various operating conditions

Auteurs : K. H. Kim [États-Unis] ; Y. S. Choi [États-Unis] ; N. P. Barnes ; R. V. Hess ; C. H. Bair ; P. Brockman

Source :

Applied optics [ 0003-6935 ] ; 1993.

RBID : Pascal:93-0614742

Descripteurs français

Pascal (Inist)
- Pompage optique, Lampe éclair, Laser solide, Laser IR, Rayonnement IR, Laser déclenché, Chrome, Thulium, Holmium, Aluminium Yttrium Oxyde Mixte.
Wicri :
- topic : Chrome.

English descriptors

KwdEn :
- Aluminium Yttrium Oxides Mixed, Chromium, Holmium, Infrared laser, Infrared radiation, Optical pumping, Photoflash lamp, Q switched laser, Solid state laser, Thulium.

Abstract

Flash-lamp-pumped normal-mode and Q-switched 2.1-μm laser operations of Ho:Tm:Cr:YAG crystals have been evaluated under a wide variety of experimental conditions in order to determine an optimum lasing condition and to characterize the laser outputs. Q-switched laser-output energies equal to or in some cases more than the normal-mode laser energies were obtained in the form of a strong single spike by optimizing the opening time of a lithium niobate Q switch. The increase of the normal-mode laser slope efficiency was observed with the increase of the Tm concentration from 2.5 to 4.5 at.% at operating temperatures from 120 K to near room temperature. Laser transitions were observed only at 2.098 and 2.091 μm under various conditions

A01	`01`	`1`		`@0 0003-6935`
A02	`01`			`@0 APOPAI`
A03		`1`		`@0 Appl. opt.`
A05				`@2 32`
A06				`@2 12`
A08	`01`	`1`	`ENG`	`@1 Investigation of 2.1-μm lasing properties of Ho:Tm:Cr:YAG crystals under flash-lamp pumping at various operating conditions`
A11	`01`	`1`		`@1 KIM (K. H.)`
A11	`02`	`1`		`@1 CHOI (Y. S.)`
A11	`03`	`1`		`@1 BARNES (N. P.)`
A11	`04`	`1`		`@1 HESS (R. V.)`
A11	`05`	`1`		`@1 BAIR (C. H.)`
A11	`06`	`1`		`@1 BROCKMAN (P.)`
A14	`01`			`@1 Hampton univ., dep. physics @2 Hampton VA 23668 @3 USA @Z 1 aut. @Z 2 aut.`
A20				`@1 2066-2074`
A21				`@1 1993`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 6309 @5 354000036301840110`
A44				`@0 0000`
A45				`@0 38 ref.`
A47	`01`	`1`		`@0 93-0614742`
A60				`@1 P`
A61				`@0 A`
A64		`1`		`@0 Applied optics`
A66	`01`			`@0 USA`
C01	`01`		`ENG`	@0 Flash-lamp-pumped normal-mode and Q-switched 2.1-μm laser operations of Ho:Tm:Cr:YAG crystals have been evaluated under a wide variety of experimental conditions in order to determine an optimum lasing condition and to characterize the laser outputs. Q-switched laser-output energies equal to or in some cases more than the normal-mode laser energies were obtained in the form of a strong single spike by optimizing the opening time of a lithium niobate Q switch. The increase of the normal-mode laser slope efficiency was observed with the increase of the Tm concentration from 2.5 to 4.5 at.% at operating temperatures from 120 K to near room temperature. Laser transitions were observed only at 2.098 and 2.091 μm under various conditions
C02	`01`	`X`		`@0 001B04G08`
C03	`01`	`X`	`FRE`	`@0 Pompage optique @5 36`
C03	`01`	`X`	`ENG`	`@0 Optical pumping @5 36`
C03	`01`	`X`	`SPA`	`@0 Bombeo óptico @5 36`
C03	`02`	`X`	`FRE`	`@0 Lampe éclair @5 37`
C03	`02`	`X`	`ENG`	`@0 Photoflash lamp @5 37`
C03	`02`	`X`	`SPA`	`@0 Lámpara relámpago @5 37`
C03	`03`	`X`	`FRE`	`@0 Laser solide @5 39`
C03	`03`	`X`	`ENG`	`@0 Solid state laser @5 39`
C03	`03`	`X`	`SPA`	`@0 Laser sólido @5 39`
C03	`04`	`X`	`FRE`	`@0 Laser IR @5 40`
C03	`04`	`X`	`ENG`	`@0 Infrared laser @5 40`
C03	`04`	`X`	`SPA`	`@0 Laser IR @5 40`
C03	`05`	`X`	`FRE`	`@0 Rayonnement IR @5 41`
C03	`05`	`X`	`ENG`	`@0 Infrared radiation @5 41`
C03	`05`	`X`	`GER`	`@0 Infrarotstrahlen @5 41`
C03	`05`	`X`	`SPA`	`@0 Radiación infrarroja @5 41`
C03	`06`	`X`	`FRE`	`@0 Laser déclenché @5 42`
C03	`06`	`X`	`ENG`	`@0 Q switched laser @5 42`
C03	`06`	`X`	`SPA`	`@0 Laser disparado @5 42`
C03	`07`	`X`	`FRE`	`@0 Chrome @1 SEC @2 NC @2 FX @5 79`
C03	`07`	`X`	`ENG`	`@0 Chromium @1 SEC @2 NC @2 FX @5 79`
C03	`07`	`X`	`GER`	`@0 Chrom @1 SEC @2 NC @2 FX @5 79`
C03	`07`	`X`	`SPA`	`@0 Cromo @1 SEC @2 NC @2 FX @5 79`
C03	`08`	`X`	`FRE`	`@0 Thulium @1 SEC @2 NC @5 80`
C03	`08`	`X`	`ENG`	`@0 Thulium @1 SEC @2 NC @5 80`
C03	`08`	`X`	`GER`	`@0 Thulium @1 SEC @2 NC @5 80`
C03	`08`	`X`	`SPA`	`@0 Tulio @1 SEC @2 NC @5 80`
C03	`09`	`X`	`FRE`	`@0 Holmium @1 SEC @2 NC @5 81`
C03	`09`	`X`	`ENG`	`@0 Holmium @1 SEC @2 NC @5 81`
C03	`09`	`X`	`GER`	`@0 Holmium @1 SEC @2 NC @5 81`
C03	`09`	`X`	`SPA`	`@0 Holmio @1 SEC @2 NC @5 81`
C03	`10`	`X`	`FRE`	`@0 Aluminium Yttrium Oxyde Mixte @1 SUB @2 NC @2 FR @2 FX @2 NA @5 82`
C03	`10`	`X`	`ENG`	`@0 Aluminium Yttrium Oxides Mixed @1 SUB @2 NC @2 FR @2 FX @2 NA @5 82`
C03	`10`	`X`	`SPA`	`@0 Aluminio Ytrio Óxido Mixto @1 SUB @2 NC @2 FR @2 FX @2 NA @5 82`
N21				`@1 292`

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Pascal:93-0614742

Le document en format XML

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<author><name sortKey="Kim, K H" sort="Kim, K H" uniqKey="Kim K" first="K. H." last="Kim">K. H. Kim</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Hampton univ., dep. physics</s1>
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<country>États-Unis</country>
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<author><name sortKey="Barnes, N P" sort="Barnes, N P" uniqKey="Barnes N" first="N. P." last="Barnes">N. P. Barnes</name>
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<author><name sortKey="Hess, R V" sort="Hess, R V" uniqKey="Hess R" first="R. V." last="Hess">R. V. Hess</name>
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<author><name sortKey="Bair, C H" sort="Bair, C H" uniqKey="Bair C" first="C. H." last="Bair">C. H. Bair</name>
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<author><name sortKey="Brockman, P" sort="Brockman, P" uniqKey="Brockman P" first="P." last="Brockman">P. Brockman</name>
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<author><name sortKey="Choi, Y S" sort="Choi, Y S" uniqKey="Choi Y" first="Y. S." last="Choi">Y. S. Choi</name>
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<author><name sortKey="Barnes, N P" sort="Barnes, N P" uniqKey="Barnes N" first="N. P." last="Barnes">N. P. Barnes</name>
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<author><name sortKey="Bair, C H" sort="Bair, C H" uniqKey="Bair C" first="C. H." last="Bair">C. H. Bair</name>
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<series><title level="j" type="main">Applied optics</title>
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<idno type="ISSN">0003-6935</idno>
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<seriesStmt><title level="j" type="main">Applied optics</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Aluminium Yttrium Oxides Mixed</term>
<term>Chromium</term>
<term>Holmium</term>
<term>Infrared laser</term>
<term>Infrared radiation</term>
<term>Optical pumping</term>
<term>Photoflash lamp</term>
<term>Q switched laser</term>
<term>Solid state laser</term>
<term>Thulium</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Pompage optique</term>
<term>Lampe éclair</term>
<term>Laser solide</term>
<term>Laser IR</term>
<term>Rayonnement IR</term>
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<term>Chrome</term>
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<term>Holmium</term>
<term>Aluminium Yttrium Oxyde Mixte</term>
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<front><div type="abstract" xml:lang="en">Flash-lamp-pumped normal-mode and Q-switched 2.1-μm laser operations of Ho:Tm:Cr:YAG crystals have been evaluated under a wide variety of experimental conditions in order to determine an optimum lasing condition and to characterize the laser outputs. Q-switched laser-output energies equal to or in some cases more than the normal-mode laser energies were obtained in the form of a strong single spike by optimizing the opening time of a lithium niobate Q switch. The increase of the normal-mode laser slope efficiency was observed with the increase of the Tm concentration from 2.5 to 4.5 at.% at operating temperatures from 120 K to near room temperature. Laser transitions were observed only at 2.098 and 2.091 μm under various conditions</div>
</front>
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<fA14 i1="01"><s1>Hampton univ., dep. physics</s1>
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<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>Flash-lamp-pumped normal-mode and Q-switched 2.1-μm laser operations of Ho:Tm:Cr:YAG crystals have been evaluated under a wide variety of experimental conditions in order to determine an optimum lasing condition and to characterize the laser outputs. Q-switched laser-output energies equal to or in some cases more than the normal-mode laser energies were obtained in the form of a strong single spike by optimizing the opening time of a lithium niobate Q switch. The increase of the normal-mode laser slope efficiency was observed with the increase of the Tm concentration from 2.5 to 4.5 at.% at operating temperatures from 120 K to near room temperature. Laser transitions were observed only at 2.098 and 2.091 μm under various conditions</s0>
</fC01>
<fC02 i1="01" i2="X"><s0>001B04G08</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Pompage optique</s0>
<s5>36</s5>
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<s5>36</s5>
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<s5>36</s5>
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<s5>37</s5>
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<s5>37</s5>
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<s5>37</s5>
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<s5>39</s5>
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<s5>39</s5>
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<s5>39</s5>
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<fC03 i1="04" i2="X" l="FRE"><s0>Laser IR</s0>
<s5>40</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Infrared laser</s0>
<s5>40</s5>
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<fC03 i1="04" i2="X" l="SPA"><s0>Laser IR</s0>
<s5>40</s5>
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<fC03 i1="05" i2="X" l="FRE"><s0>Rayonnement IR</s0>
<s5>41</s5>
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<fC03 i1="05" i2="X" l="ENG"><s0>Infrared radiation</s0>
<s5>41</s5>
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<fC03 i1="05" i2="X" l="GER"><s0>Infrarotstrahlen</s0>
<s5>41</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Radiación infrarroja</s0>
<s5>41</s5>
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<fC03 i1="06" i2="X" l="FRE"><s0>Laser déclenché</s0>
<s5>42</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Q switched laser</s0>
<s5>42</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Laser disparado</s0>
<s5>42</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Chrome</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s2>FX</s2>
<s5>79</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Chromium</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s2>FX</s2>
<s5>79</s5>
</fC03>
<fC03 i1="07" i2="X" l="GER"><s0>Chrom</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s2>FX</s2>
<s5>79</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Cromo</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s2>FX</s2>
<s5>79</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Thulium</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s5>80</s5>
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<fC03 i1="08" i2="X" l="ENG"><s0>Thulium</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s5>80</s5>
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<fC03 i1="08" i2="X" l="GER"><s0>Thulium</s0>
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<s1>SEC</s1>
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<s5>81</s5>
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<s1>SEC</s1>
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<s5>81</s5>
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<fC03 i1="09" i2="X" l="SPA"><s0>Holmio</s0>
<s1>SEC</s1>
<s2>NC</s2>
<s5>81</s5>
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<fC03 i1="10" i2="X" l="FRE"><s0>Aluminium Yttrium Oxyde Mixte</s0>
<s1>SUB</s1>
<s2>NC</s2>
<s2>FR</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>82</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Aluminium Yttrium Oxides Mixed</s0>
<s1>SUB</s1>
<s2>NC</s2>
<s2>FR</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>82</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Aluminio Ytrio Óxido Mixto</s0>
<s1>SUB</s1>
<s2>NC</s2>
<s2>FR</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>82</s5>
</fC03>
<fN21><s1>292</s1>
</fN21>
</pA>
</standard>
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</record>

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Investigation of 2.1-μm lasing properties of Ho:Tm:Cr:YAG crystals under flash-lamp pumping at various operating conditions

Investigation of 2.1-μm lasing properties of Ho:Tm:Cr:YAG crystals under flash-lamp pumping at various operating conditions

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