High-power linearly-polarized single-frequency thulium-doped fiber Master-Oscillator Power-Amplifier.
Identifieur interne : 000496 ( PubMed/Corpus ); précédent : 000495; suivant : 000497High-power linearly-polarized single-frequency thulium-doped fiber Master-Oscillator Power-Amplifier.
Auteurs : L. Pearson ; J W Kim ; Z. Zhang ; M. Ibsen ; J K Sahu ; W A ClarksonSource :
- Optics express [ 1094-4087 ] ; 2010.
English descriptors
- KwdEn :
- MESH :
- chemical , chemistry : Thulium.
- instrumentation : Fiber Optic Technology, Oscillometry, Refractometry.
- Equipment Design, Equipment Failure Analysis, Linear Models, Optical Devices.
Abstract
We report a high power narrow-linewidth source at approximately 2 microm based on a Tm-doped fiber distributed-feedback master-oscillator and three Tm fiber amplifier stages. The master-oscillator and first two amplifier stages were in-band pumped by Er,Yb fiber lasers operating at 1565 nm, and the final stage amplifier was cladding-pumped at 795 nm by two spatially-combined diode-stacks. The MOPA yielded 100 W of single frequency output at 1943 nm with a beam propagation factor (M(2)) of 1.25 and with a polarization extinction ratio of >94%. The output power was limited by thermally-induced damage in the final amplifier stage. The prospects for further power scaling are considered.
PubMed: 20173987
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pubmed:20173987Le document en format XML
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<author><name sortKey="Kim, J W" sort="Kim, J W" uniqKey="Kim J" first="J W" last="Kim">J W Kim</name>
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<author><name sortKey="Zhang, Z" sort="Zhang, Z" uniqKey="Zhang Z" first="Z" last="Zhang">Z. Zhang</name>
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<author><name sortKey="Ibsen, M" sort="Ibsen, M" uniqKey="Ibsen M" first="M" last="Ibsen">M. Ibsen</name>
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<author><name sortKey="Sahu, J K" sort="Sahu, J K" uniqKey="Sahu J" first="J K" last="Sahu">J K Sahu</name>
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<author><name sortKey="Clarkson, W A" sort="Clarkson, W A" uniqKey="Clarkson W" first="W A" last="Clarkson">W A Clarkson</name>
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<author><name sortKey="Pearson, L" sort="Pearson, L" uniqKey="Pearson L" first="L" last="Pearson">L. Pearson</name>
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<author><name sortKey="Zhang, Z" sort="Zhang, Z" uniqKey="Zhang Z" first="Z" last="Zhang">Z. Zhang</name>
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<author><name sortKey="Ibsen, M" sort="Ibsen, M" uniqKey="Ibsen M" first="M" last="Ibsen">M. Ibsen</name>
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<author><name sortKey="Sahu, J K" sort="Sahu, J K" uniqKey="Sahu J" first="J K" last="Sahu">J K Sahu</name>
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<author><name sortKey="Clarkson, W A" sort="Clarkson, W A" uniqKey="Clarkson W" first="W A" last="Clarkson">W A Clarkson</name>
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<series><title level="j">Optics express</title>
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<term>Linear Models</term>
<term>Optical Devices</term>
<term>Oscillometry (instrumentation)</term>
<term>Refractometry (instrumentation)</term>
<term>Thulium (chemistry)</term>
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<keywords scheme="MESH" qualifier="instrumentation" xml:lang="en"><term>Fiber Optic Technology</term>
<term>Oscillometry</term>
<term>Refractometry</term>
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<front><div type="abstract" xml:lang="en">We report a high power narrow-linewidth source at approximately 2 microm based on a Tm-doped fiber distributed-feedback master-oscillator and three Tm fiber amplifier stages. The master-oscillator and first two amplifier stages were in-band pumped by Er,Yb fiber lasers operating at 1565 nm, and the final stage amplifier was cladding-pumped at 795 nm by two spatially-combined diode-stacks. The MOPA yielded 100 W of single frequency output at 1943 nm with a beam propagation factor (M(2)) of 1.25 and with a polarization extinction ratio of >94%. The output power was limited by thermally-induced damage in the final amplifier stage. The prospects for further power scaling are considered.</div>
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<Abstract><AbstractText>We report a high power narrow-linewidth source at approximately 2 microm based on a Tm-doped fiber distributed-feedback master-oscillator and three Tm fiber amplifier stages. The master-oscillator and first two amplifier stages were in-band pumped by Er,Yb fiber lasers operating at 1565 nm, and the final stage amplifier was cladding-pumped at 795 nm by two spatially-combined diode-stacks. The MOPA yielded 100 W of single frequency output at 1943 nm with a beam propagation factor (M(2)) of 1.25 and with a polarization extinction ratio of >94%. The output power was limited by thermally-induced damage in the final amplifier stage. The prospects for further power scaling are considered.</AbstractText>
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