Monolithic, narrow linewidth, polarization maintaining, thulium fiber laser using femtosecond laser written fiber Bragg gratings
Identifieur interne :
000189 ( Pascal/Curation );
précédent :
000188;
suivant :
000190
Monolithic, narrow linewidth, polarization maintaining, thulium fiber laser using femtosecond laser written fiber Bragg gratings
Auteurs : Christina C. C. Willis [
États-Unis] ;
Joshua D. Bradford [
États-Unis] ;
R. Andrew Sims [
États-Unis] ;
Lawrence Shah [
États-Unis] ;
Martin Richardson [
États-Unis] ;
Jens Thomas [
Allemagne] ;
Ria G. Becker [
Allemagne] ;
Christian Voigtl Nder [
Allemagne] ;
Andreas Tünnermann [
Allemagne] ;
Stefan Nolte [
Allemagne]
Source :
-
Proceedings of SPIE, the International Society for Optical Engineering [ 0277-786X ] ; 2011.
RBID : Pascal:12-0011741
Descripteurs français
- Pascal (Inist)
- Réseau diffraction,
Laser fibre,
Laser pulsé,
Réseau dans fibre,
Réseau Bragg,
Intracavité,
Elément optique,
Application laser,
Largeur raie,
Domaine temps fs,
Facteur réflexion,
Puissance sortie,
Fibre optique,
Silice,
Thulium,
Application militaire,
0130C,
4262,
4255W,
4281W,
8920D,
4279D.
English descriptors
- KwdEn :
- Bragg gratings,
Diffraction gratings,
Fiber lasers,
Grating in fiber,
Intracavity,
Laser beam applications,
Line widths,
Military application,
Optical elements,
Optical fibers,
Output power,
Pulsed lasers,
Reflectivity,
Silica,
Thulium,
fs range.
Abstract
We have demonstrated an all-fiber thulium laser system that, without any intracavity polarizing elements or free-space components, yielded a stable polarization extinction ratio (PER) of ∼18 dB. The system is based on single-mode polarization-maintaining silica fiber and its cavity is formed from each a high and low reflectivity femtosecond laser written fiber Bragg grating resonant at 2054 nm. The output of the fiber is not only highly polarized, but maintains a narrow linewidth of 78 pm at its maximum output power of 5.24 W. The high PER without any polarizing elements in the cavity is of great interest and makes the systems useful for spectral beam combining and other applications which require polarization dependent optical elements.
| pA |
| A01 | 01 | 1 | | @0 0277-786X |
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| A02 | 01 | | | @0 PSISDG |
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| A03 | | 1 | | @0 Proc. SPIE Int. Soc. Opt. Eng. |
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| A05 | | | | @2 8039 |
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| A08 | 01 | 1 | ENG | @1 Monolithic, narrow linewidth, polarization maintaining, thulium fiber laser using femtosecond laser written fiber Bragg gratings |
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| A09 | 01 | 1 | ENG | @1 Laser technology for defense and security VII : 25-27 April 2011, Orlando, Florida, United States |
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| A11 | 01 | 1 | | @1 WILLIS (Christina C. C.) |
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| A11 | 02 | 1 | | @1 BRADFORD (Joshua D.) |
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| A11 | 03 | 1 | | @1 SIMS (R. Andrew) |
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| A11 | 04 | 1 | | @1 SHAH (Lawrence) |
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| A11 | 05 | 1 | | @1 RICHARDSON (Martin) |
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| A11 | 06 | 1 | | @1 THOMAS (Jens) |
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| A11 | 07 | 1 | | @1 BECKER (Ria G.) |
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| A11 | 08 | 1 | | @1 VOIGTLÄNDER (Christian) |
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| A11 | 09 | 1 | | @1 TÜNNERMANN (Andreas) |
|---|
| A11 | 10 | 1 | | @1 NOLTE (Stefan) |
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| A12 | 01 | 1 | | @1 DUBINSKII (Mark A.) @9 ed. |
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| A12 | 02 | 1 | | @1 POST (Stephen G.) @9 ed. |
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| A14 | 01 | | | @1 Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard @2 Orlando, Florida 32816 @3 USA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. |
|---|
| A14 | 02 | | | @1 Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15 @2 07745 Jena @3 DEU @Z 6 aut. @Z 7 aut. @Z 8 aut. @Z 9 aut. @Z 10 aut. |
|---|
| A14 | 03 | | | @1 Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7 @2 07745 Jena @3 DEU @Z 9 aut. @Z 10 aut. |
|---|
| A18 | 01 | 1 | | @1 SPIE @3 USA @9 org-cong. |
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| A20 | | | | @2 80390H.1-80390H.6 |
|---|
| A21 | | | | @1 2011 |
|---|
| A23 | 01 | | | @0 ENG |
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| A25 | 01 | | | @1 SPIE @2 Bellingham WA |
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| A26 | 01 | | | @0 978-0-8194-8613-4 |
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| A43 | 01 | | | @1 INIST @2 21760 @5 354000174755190100 |
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| A44 | | | | @0 0000 @1 © 2012 INIST-CNRS. All rights reserved. |
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| A45 | | | | @0 16 ref. |
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| A47 | 01 | 1 | | @0 12-0011741 |
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| A60 | | | | @1 P @2 C |
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| A61 | | | | @0 A |
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| A64 | 01 | 1 | | @0 Proceedings of SPIE, the International Society for Optical Engineering |
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| A66 | 01 | | | @0 USA |
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| C01 | 01 | | ENG | @0 We have demonstrated an all-fiber thulium laser system that, without any intracavity polarizing elements or free-space components, yielded a stable polarization extinction ratio (PER) of ∼18 dB. The system is based on single-mode polarization-maintaining silica fiber and its cavity is formed from each a high and low reflectivity femtosecond laser written fiber Bragg grating resonant at 2054 nm. The output of the fiber is not only highly polarized, but maintains a narrow linewidth of 78 pm at its maximum output power of 5.24 W. The high PER without any polarizing elements in the cavity is of great interest and makes the systems useful for spectral beam combining and other applications which require polarization dependent optical elements. |
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| C02 | 01 | 3 | | @0 001B00A30C |
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| C02 | 02 | 3 | | @0 001B40B62 |
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| C02 | 03 | 3 | | @0 001B40B55W |
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| C02 | 04 | 3 | | @0 001B40B81W |
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| C03 | 01 | 3 | FRE | @0 Réseau diffraction @5 09 |
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| C03 | 01 | 3 | ENG | @0 Diffraction gratings @5 09 |
|---|
| C03 | 02 | 3 | FRE | @0 Laser fibre @5 11 |
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| C03 | 02 | 3 | ENG | @0 Fiber lasers @5 11 |
|---|
| C03 | 03 | 3 | FRE | @0 Laser pulsé @5 12 |
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| C03 | 03 | 3 | ENG | @0 Pulsed lasers @5 12 |
|---|
| C03 | 04 | X | FRE | @0 Réseau dans fibre @5 13 |
|---|
| C03 | 04 | X | ENG | @0 Grating in fiber @5 13 |
|---|
| C03 | 04 | X | SPA | @0 Red en fibra @5 13 |
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| C03 | 05 | 3 | FRE | @0 Réseau Bragg @5 14 |
|---|
| C03 | 05 | 3 | ENG | @0 Bragg gratings @5 14 |
|---|
| C03 | 06 | X | FRE | @0 Intracavité @5 15 |
|---|
| C03 | 06 | X | ENG | @0 Intracavity @5 15 |
|---|
| C03 | 06 | X | SPA | @0 Cavidad interna @5 15 |
|---|
| C03 | 07 | 3 | FRE | @0 Elément optique @5 16 |
|---|
| C03 | 07 | 3 | ENG | @0 Optical elements @5 16 |
|---|
| C03 | 08 | 3 | FRE | @0 Application laser @5 19 |
|---|
| C03 | 08 | 3 | ENG | @0 Laser beam applications @5 19 |
|---|
| C03 | 09 | 3 | FRE | @0 Largeur raie @5 41 |
|---|
| C03 | 09 | 3 | ENG | @0 Line widths @5 41 |
|---|
| C03 | 10 | 3 | FRE | @0 Domaine temps fs @5 42 |
|---|
| C03 | 10 | 3 | ENG | @0 fs range @5 42 |
|---|
| C03 | 11 | 3 | FRE | @0 Facteur réflexion @5 43 |
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| C03 | 11 | 3 | ENG | @0 Reflectivity @5 43 |
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| C03 | 12 | X | FRE | @0 Puissance sortie @5 44 |
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| C03 | 12 | X | ENG | @0 Output power @5 44 |
|---|
| C03 | 12 | X | SPA | @0 Potencia salida @5 44 |
|---|
| C03 | 13 | 3 | FRE | @0 Fibre optique @5 47 |
|---|
| C03 | 13 | 3 | ENG | @0 Optical fibers @5 47 |
|---|
| C03 | 14 | 3 | FRE | @0 Silice @2 NK @5 57 |
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| C03 | 14 | 3 | ENG | @0 Silica @2 NK @5 57 |
|---|
| C03 | 15 | 3 | FRE | @0 Thulium @2 NC @5 61 |
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| C03 | 15 | 3 | ENG | @0 Thulium @2 NC @5 61 |
|---|
| C03 | 16 | X | FRE | @0 Application militaire @5 62 |
|---|
| C03 | 16 | X | ENG | @0 Military application @5 62 |
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| C03 | 16 | X | SPA | @0 Aplicación militar @5 62 |
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| C03 | 17 | 3 | FRE | @0 0130C @4 INC @5 83 |
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| C03 | 18 | 3 | FRE | @0 4262 @4 INC @5 84 |
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| C03 | 19 | 3 | FRE | @0 4255W @4 INC @5 91 |
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| C03 | 20 | 3 | FRE | @0 4281W @4 INC @5 92 |
|---|
| C03 | 21 | 3 | FRE | @0 8920D @4 INC @5 93 |
|---|
| C03 | 22 | 3 | FRE | @0 4279D @4 INC @5 94 |
|---|
| N21 | | | | @1 002 |
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| N44 | 01 | | | @1 OTO |
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| N82 | | | | @1 OTO |
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|
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| pR |
| A30 | 01 | 1 | ENG | @1 Laser technology for defense and security. Conference @2 07 @3 Orlando FL USA @4 2011-04-25 |
|---|
|
|---|
Links toward previous steps (curation, corpus...)
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Pascal:12-0011741
Le document en format XML
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</affiliation><author><name sortKey="Becker, Ria G" sort="Becker, Ria G" uniqKey="Becker R" first="Ria G." last="Becker">Ria G. Becker</name>
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<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Voigtl Nder, Christian" sort="Voigtl Nder, Christian" uniqKey="Voigtl Nder C" first="Christian" last="Voigtl Nder">Christian Voigtl Nder</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Tunnermann, Andreas" sort="Tunnermann, Andreas" uniqKey="Tunnermann A" first="Andreas" last="Tünnermann">Andreas Tünnermann</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Nolte, Stefan" sort="Nolte, Stefan" uniqKey="Nolte S" first="Stefan" last="Nolte">Stefan Nolte</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><publicationStmt><idno type="wicri:source">INIST</idno>
<idno type="inist">12-0011741</idno>
<date when="2011">2011</date>
<idno type="stanalyst">PASCAL 12-0011741 INIST</idno>
<idno type="RBID">Pascal:12-0011741</idno>
<idno type="wicri:Area/Pascal/Corpus">000189</idno>
<idno type="wicri:Area/Pascal/Curation">000189</idno>
</publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Monolithic, narrow linewidth, polarization maintaining, thulium fiber laser using femtosecond laser written fiber Bragg gratings</title>
<author><name sortKey="Willis, Christina C C" sort="Willis, Christina C C" uniqKey="Willis C" first="Christina C. C." last="Willis">Christina C. C. Willis</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Bradford, Joshua D" sort="Bradford, Joshua D" uniqKey="Bradford J" first="Joshua D." last="Bradford">Joshua D. Bradford</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Sims, R Andrew" sort="Sims, R Andrew" uniqKey="Sims R" first="R. Andrew" last="Sims">R. Andrew Sims</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Shah, Lawrence" sort="Shah, Lawrence" uniqKey="Shah L" first="Lawrence" last="Shah">Lawrence Shah</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Richardson, Martin" sort="Richardson, Martin" uniqKey="Richardson M" first="Martin" last="Richardson">Martin Richardson</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Thomas, Jens" sort="Thomas, Jens" uniqKey="Thomas J" first="Jens" last="Thomas">Jens Thomas</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Becker, Ria G" sort="Becker, Ria G" uniqKey="Becker R" first="Ria G." last="Becker">Ria G. Becker</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Voigtl Nder, Christian" sort="Voigtl Nder, Christian" uniqKey="Voigtl Nder C" first="Christian" last="Voigtl Nder">Christian Voigtl Nder</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Tunnermann, Andreas" sort="Tunnermann, Andreas" uniqKey="Tunnermann A" first="Andreas" last="Tünnermann">Andreas Tünnermann</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><author><name sortKey="Nolte, Stefan" sort="Nolte, Stefan" uniqKey="Nolte S" first="Stefan" last="Nolte">Stefan Nolte</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</inist:fA14><country>Allemagne</country>
</affiliation><series><title level="j" type="main">Proceedings of SPIE, the International Society for Optical Engineering</title>
<title level="j" type="abbreviated">Proc. SPIE Int. Soc. Opt. Eng.</title>
<idno type="ISSN">0277-786X</idno>
<imprint><date when="2011">2011</date>
</imprint><seriesStmt><title level="j" type="main">Proceedings of SPIE, the International Society for Optical Engineering</title>
<title level="j" type="abbreviated">Proc. SPIE Int. Soc. Opt. Eng.</title>
<idno type="ISSN">0277-786X</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Bragg gratings</term>
<term>Diffraction gratings</term>
<term>Fiber lasers</term>
<term>Grating in fiber</term>
<term>Intracavity</term>
<term>Laser beam applications</term>
<term>Line widths</term>
<term>Military application</term>
<term>Optical elements</term>
<term>Optical fibers</term>
<term>Output power</term>
<term>Pulsed lasers</term>
<term>Reflectivity</term>
<term>Silica</term>
<term>Thulium</term>
<term>fs range</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Réseau diffraction</term>
<term>Laser fibre</term>
<term>Laser pulsé</term>
<term>Réseau dans fibre</term>
<term>Réseau Bragg</term>
<term>Intracavité</term>
<term>Elément optique</term>
<term>Application laser</term>
<term>Largeur raie</term>
<term>Domaine temps fs</term>
<term>Facteur réflexion</term>
<term>Puissance sortie</term>
<term>Fibre optique</term>
<term>Silice</term>
<term>Thulium</term>
<term>Application militaire</term>
<term>0130C</term>
<term>4262</term>
<term>4255W</term>
<term>4281W</term>
<term>8920D</term>
<term>4279D</term>
</keywords><front><div type="abstract" xml:lang="en">We have demonstrated an all-fiber thulium laser system that, without any intracavity polarizing elements or free-space components, yielded a stable polarization extinction ratio (PER) of ∼18 dB. The system is based on single-mode polarization-maintaining silica fiber and its cavity is formed from each a high and low reflectivity femtosecond laser written fiber Bragg grating resonant at 2054 nm. The output of the fiber is not only highly polarized, but maintains a narrow linewidth of 78 pm at its maximum output power of 5.24 W. The high PER without any polarizing elements in the cavity is of great interest and makes the systems useful for spectral beam combining and other applications which require polarization dependent optical elements.</div>
</front><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0277-786X</s0>
</fA01><fA02 i1="01"><s0>PSISDG</s0>
</fA02><fA03 i2="1"><s0>Proc. SPIE Int. Soc. Opt. Eng.</s0>
</fA03><fA05><s2>8039</s2>
</fA05><fA08 i1="01" i2="1" l="ENG"><s1>Monolithic, narrow linewidth, polarization maintaining, thulium fiber laser using femtosecond laser written fiber Bragg gratings</s1>
</fA08><fA09 i1="01" i2="1" l="ENG"><s1>Laser technology for defense and security VII : 25-27 April 2011, Orlando, Florida, United States</s1>
</fA09><fA11 i1="01" i2="1"><s1>WILLIS (Christina C. C.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>BRADFORD (Joshua D.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>SIMS (R. Andrew)</s1>
</fA11><fA11 i1="04" i2="1"><s1>SHAH (Lawrence)</s1>
</fA11><fA11 i1="05" i2="1"><s1>RICHARDSON (Martin)</s1>
</fA11><fA11 i1="06" i2="1"><s1>THOMAS (Jens)</s1>
</fA11><fA11 i1="07" i2="1"><s1>BECKER (Ria G.)</s1>
</fA11><fA11 i1="08" i2="1"><s1>VOIGTLÄNDER (Christian)</s1>
</fA11><fA11 i1="09" i2="1"><s1>TÜNNERMANN (Andreas)</s1>
</fA11><fA11 i1="10" i2="1"><s1>NOLTE (Stefan)</s1>
</fA11><fA12 i1="01" i2="1"><s1>DUBINSKII (Mark A.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="02" i2="1"><s1>POST (Stephen G.)</s1>
<s9>ed.</s9>
</fA12><fA14 i1="01"><s1>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard</s1>
<s2>Orlando, Florida 32816</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14><fA14 i1="02"><s1>Institute of Applied Physics, Friedrich-Schiller-University, Albert-Einstein-Strasse 15</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</fA14><fA14 i1="03"><s1>Fraunhofer Institute for Applied Optics and Precision Engineering, Albert-Einstein-Str. 7</s1>
<s2>07745 Jena</s2>
<s3>DEU</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</fA14><fA18 i1="01" i2="1"><s1>SPIE</s1>
<s3>USA</s3>
<s9>org-cong.</s9>
</fA18><fA20><s2>80390H.1-80390H.6</s2>
</fA20><fA21><s1>2011</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA25 i1="01"><s1>SPIE</s1>
<s2>Bellingham WA</s2>
</fA25><fA26 i1="01"><s0>978-0-8194-8613-4</s0>
</fA26><fA43 i1="01"><s1>INIST</s1>
<s2>21760</s2>
<s5>354000174755190100</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>16 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>12-0011741</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>Proceedings of SPIE, the International Society for Optical Engineering</s0>
</fA64><fA66 i1="01"><s0>USA</s0>
</fA66><fC01 i1="01" l="ENG"><s0>We have demonstrated an all-fiber thulium laser system that, without any intracavity polarizing elements or free-space components, yielded a stable polarization extinction ratio (PER) of ∼18 dB. The system is based on single-mode polarization-maintaining silica fiber and its cavity is formed from each a high and low reflectivity femtosecond laser written fiber Bragg grating resonant at 2054 nm. The output of the fiber is not only highly polarized, but maintains a narrow linewidth of 78 pm at its maximum output power of 5.24 W. The high PER without any polarizing elements in the cavity is of great interest and makes the systems useful for spectral beam combining and other applications which require polarization dependent optical elements.</s0>
</fC01><fC02 i1="01" i2="3"><s0>001B00A30C</s0>
</fC02><fC02 i1="02" i2="3"><s0>001B40B62</s0>
</fC02><fC02 i1="03" i2="3"><s0>001B40B55W</s0>
</fC02><fC02 i1="04" i2="3"><s0>001B40B81W</s0>
</fC02><fC03 i1="01" i2="3" l="FRE"><s0>Réseau diffraction</s0>
<s5>09</s5>
</fC03><fC03 i1="01" i2="3" l="ENG"><s0>Diffraction gratings</s0>
<s5>09</s5>
</fC03><fC03 i1="02" i2="3" l="FRE"><s0>Laser fibre</s0>
<s5>11</s5>
</fC03><fC03 i1="02" i2="3" l="ENG"><s0>Fiber lasers</s0>
<s5>11</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Laser pulsé</s0>
<s5>12</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>Pulsed lasers</s0>
<s5>12</s5>
</fC03><fC03 i1="04" i2="X" l="FRE"><s0>Réseau dans fibre</s0>
<s5>13</s5>
</fC03><fC03 i1="04" i2="X" l="ENG"><s0>Grating in fiber</s0>
<s5>13</s5>
</fC03><fC03 i1="04" i2="X" l="SPA"><s0>Red en fibra</s0>
<s5>13</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Réseau Bragg</s0>
<s5>14</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Bragg gratings</s0>
<s5>14</s5>
</fC03><fC03 i1="06" i2="X" l="FRE"><s0>Intracavité</s0>
<s5>15</s5>
</fC03><fC03 i1="06" i2="X" l="ENG"><s0>Intracavity</s0>
<s5>15</s5>
</fC03><fC03 i1="06" i2="X" l="SPA"><s0>Cavidad interna</s0>
<s5>15</s5>
</fC03><fC03 i1="07" i2="3" l="FRE"><s0>Elément optique</s0>
<s5>16</s5>
</fC03><fC03 i1="07" i2="3" l="ENG"><s0>Optical elements</s0>
<s5>16</s5>
</fC03><fC03 i1="08" i2="3" l="FRE"><s0>Application laser</s0>
<s5>19</s5>
</fC03><fC03 i1="08" i2="3" l="ENG"><s0>Laser beam applications</s0>
<s5>19</s5>
</fC03><fC03 i1="09" i2="3" l="FRE"><s0>Largeur raie</s0>
<s5>41</s5>
</fC03><fC03 i1="09" i2="3" l="ENG"><s0>Line widths</s0>
<s5>41</s5>
</fC03><fC03 i1="10" i2="3" l="FRE"><s0>Domaine temps fs</s0>
<s5>42</s5>
</fC03><fC03 i1="10" i2="3" l="ENG"><s0>fs range</s0>
<s5>42</s5>
</fC03><fC03 i1="11" i2="3" l="FRE"><s0>Facteur réflexion</s0>
<s5>43</s5>
</fC03><fC03 i1="11" i2="3" l="ENG"><s0>Reflectivity</s0>
<s5>43</s5>
</fC03><fC03 i1="12" i2="X" l="FRE"><s0>Puissance sortie</s0>
<s5>44</s5>
</fC03><fC03 i1="12" i2="X" l="ENG"><s0>Output power</s0>
<s5>44</s5>
</fC03><fC03 i1="12" i2="X" l="SPA"><s0>Potencia salida</s0>
<s5>44</s5>
</fC03><fC03 i1="13" i2="3" l="FRE"><s0>Fibre optique</s0>
<s5>47</s5>
</fC03><fC03 i1="13" i2="3" l="ENG"><s0>Optical fibers</s0>
<s5>47</s5>
</fC03><fC03 i1="14" i2="3" l="FRE"><s0>Silice</s0>
<s2>NK</s2>
<s5>57</s5>
</fC03><fC03 i1="14" i2="3" l="ENG"><s0>Silica</s0>
<s2>NK</s2>
<s5>57</s5>
</fC03><fC03 i1="15" i2="3" l="FRE"><s0>Thulium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="15" i2="3" l="ENG"><s0>Thulium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="16" i2="X" l="FRE"><s0>Application militaire</s0>
<s5>62</s5>
</fC03><fC03 i1="16" i2="X" l="ENG"><s0>Military application</s0>
<s5>62</s5>
</fC03><fC03 i1="16" i2="X" l="SPA"><s0>Aplicación militar</s0>
<s5>62</s5>
</fC03><fC03 i1="17" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03><fC03 i1="18" i2="3" l="FRE"><s0>4262</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03><fC03 i1="19" i2="3" l="FRE"><s0>4255W</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03><fC03 i1="20" i2="3" l="FRE"><s0>4281W</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03><fC03 i1="21" i2="3" l="FRE"><s0>8920D</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03><fC03 i1="22" i2="3" l="FRE"><s0>4279D</s0>
<s4>INC</s4>
<s5>94</s5>
</fC03><fN21><s1>002</s1>
</fN21><fN44 i1="01"><s1>OTO</s1>
</fN44><fN82><s1>OTO</s1>
</fN82><pR><fA30 i1="01" i2="1" l="ENG"><s1>Laser technology for defense and security. Conference</s1>
<s2>07</s2>
<s3>Orlando FL USA</s3>
<s4>2011-04-25</s4>
</fA30>
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