Frequency conversion from near-infrared to mid-infrared in highly nonlinear optical fibres
Identifieur interne : 003D81 ( PascalFrancis/Curation ); précédent : 003D80; suivant : 003D82Frequency conversion from near-infrared to mid-infrared in highly nonlinear optical fibres
Auteurs : Nicolas Ducros [France] ; Franck Morin [France] ; Kevin Cook [Australie] ; Alexis Labruyere [France] ; Sébastien Fevrier [France] ; Georges Humbert [France] ; Frédéric Druon [France] ; Marc Hanna [France] ; Patrick Georges [France] ; J. Canning [Australie] ; Ryszard Buczynski [Pologne] ; Darius Pysz [Pologne] ; Ryszard Stepien [Pologne]Source :
- Proceedings of SPIE, the International Society for Optical Engineering [ 0277-786X ] ; 2010.
Descripteurs français
- Pascal (Inist)
- Conversion fréquence optique, Diffusion Raman stimulée, Soliton optique, Déplacement fréquence, Saut indice, Impulsion ultracourte, Réseau diffraction, Réseau dans fibre, Réseau Bragg, Optique non linéaire, Indice réfraction, Subpicoseconde, Fibre optique, Fibre microstructurée, Composé binaire, Sulfure d'arsenic, Silice, Chalcogénure, Métal lourd, Oxyde métallique, Verre, Gallium, As2S3, As S, 0130C, 4265R, 4281, 4279D, 4265K, 4265D, 4265T, 4281W, Indice réfraction non linéaire.
- Wicri :
- topic : Métal lourd, Verre.
English descriptors
- KwdEn :
- Arsenic sulfides, Binary compounds, Bragg gratings, Chalcogenides, Diffraction gratings, Frequency shift, Gallium, Glass, Grating in fiber, Heavy metal, Metal oxides, Microstructured fiber, Nonlinear optics, Nonlinear refractive index, Optical fibers, Optical frequency conversion, Optical solitons, Refractive index, Silica, Step index, Stimulated Raman scattering, Subpicosecond, Ultrashort pulse.
Abstract
Chalcogenide or heavy metal oxide glasses are well known for their good transparency in the mid-infrared (MIR) domain as well as their high nonlinear refractive index (n2) tens to hundreds times higher than that of silica. We have investigated the nonlinear frequency conversion processes, based upon either stimulated Raman scattering (SRS) or soliton fission and soliton self-frequency shift (SSFS) in fibres made up with such highly nonlinear infrared transmitting glasses. First, SRS has been investigated in a chalcogenide As2S3 step index fibre. In the single pass configuration, under quasi continuous wave 1550 nm pumping, Raman cascade up to the forth Stokes order has been obtained in a 3 m long piece of fibre. The possibility to build a Raman laser thanks to in-fibre written Bragg gratings has also been investigated. A 5 dB Bragg grating has been written successfully in the core. Then, nonlinear frequency conversion in ultra-short pulse regime has been studied in a heavy metal oxide (lead-bismuth-gallium ternary system) glass photonic crystal fibre. Broadband radiation, from 800 nm up to 2.8 μm, has been obtained by pumping an 8 cm long piece of fibre at 1600 nm in sub-picosecond pulsed regime. The nonlinear frequency conversion process was assessed by numerical modelling taking into account the actual fibre cross-section as well as the measured linear and nonlinear parameters and was found to be due to soliton fission and Raman-induced SSFS.
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Links toward previous steps (curation, corpus...)
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Links to Exploration step
Pascal:11-0015340Le document en format XML
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Canning</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Interdisciplinary Photonics Laboratories, School of Chemistry, University of Sydney</s1><s2>NSW, 2006</s2><s3>AUS</s3><sZ>3 aut.</sZ><sZ>10 aut.</sZ></inist:fA14><country>Australie</country></affiliation></author><author><name sortKey="Buczynski, Ryszard" sort="Buczynski, Ryszard" uniqKey="Buczynski R" first="Ryszard" last="Buczynski">Ryszard Buczynski</name><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Faculty of Physics, University of Warsaw, Pasteura, 7</s1><s2>02-093 Warsaw</s2><s3>POL</s3><sZ>11 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Pysz, Darius" sort="Pysz, Darius" uniqKey="Pysz D" first="Darius" last="Pysz">Darius Pysz</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Glass Laboratory, Institute of Electronic Materials Technology, Wólczyńska, 133</s1><s2>01-919 Warsaw</s2><s3>POL</s3><sZ>12 aut.</sZ><sZ>13 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Stepien, Ryszard" sort="Stepien, Ryszard" uniqKey="Stepien R" first="Ryszard" last="Stepien">Ryszard Stepien</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Glass Laboratory, Institute of Electronic Materials Technology, Wólczyńska, 133</s1><s2>01-919 Warsaw</s2><s3>POL</s3><sZ>12 aut.</sZ><sZ>13 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">INIST</idno><idno type="inist">11-0015340</idno><date when="2010">2010</date><idno type="stanalyst">PASCAL 11-0015340 INIST</idno><idno type="RBID">Pascal:11-0015340</idno><idno type="wicri:Area/PascalFrancis/Corpus">002146</idno><idno type="wicri:Area/PascalFrancis/Curation">003D81</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Frequency conversion from near-infrared to mid-infrared in highly nonlinear optical fibres</title><author><name sortKey="Ducros, Nicolas" sort="Ducros, Nicolas" uniqKey="Ducros N" first="Nicolas" last="Ducros">Nicolas Ducros</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Xlim UMR CNRS 6172, 123 avenue A. Thomas</s1><s2>87060 Limoges</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Morin, Franck" sort="Morin, Franck" uniqKey="Morin F" first="Franck" last="Morin">Franck Morin</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Charles Fabry de l'Institut d'Optique, Université Paris-Sud</s1><s2>91127 Palaiseau</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>7 aut.</sZ><sZ>8 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Cook, Kevin" sort="Cook, Kevin" uniqKey="Cook K" first="Kevin" last="Cook">Kevin Cook</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Interdisciplinary Photonics Laboratories, School of Chemistry, University of Sydney</s1><s2>NSW, 2006</s2><s3>AUS</s3><sZ>3 aut.</sZ><sZ>10 aut.</sZ></inist:fA14><country>Australie</country></affiliation></author><author><name sortKey="Labruyere, Alexis" sort="Labruyere, Alexis" uniqKey="Labruyere A" first="Alexis" last="Labruyere">Alexis Labruyere</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Xlim UMR CNRS 6172, 123 avenue A. Thomas</s1><s2>87060 Limoges</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Fevrier, Sebastien" sort="Fevrier, Sebastien" uniqKey="Fevrier S" first="Sébastien" last="Fevrier">Sébastien Fevrier</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Xlim UMR CNRS 6172, 123 avenue A. Thomas</s1><s2>87060 Limoges</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Humbert, Georges" sort="Humbert, Georges" uniqKey="Humbert G" first="Georges" last="Humbert">Georges Humbert</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Xlim UMR CNRS 6172, 123 avenue A. Thomas</s1><s2>87060 Limoges</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Druon, Frederic" sort="Druon, Frederic" uniqKey="Druon F" first="Frédéric" last="Druon">Frédéric Druon</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Charles Fabry de l'Institut d'Optique, Université Paris-Sud</s1><s2>91127 Palaiseau</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>7 aut.</sZ><sZ>8 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Hanna, Marc" sort="Hanna, Marc" uniqKey="Hanna M" first="Marc" last="Hanna">Marc Hanna</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Charles Fabry de l'Institut d'Optique, Université Paris-Sud</s1><s2>91127 Palaiseau</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>7 aut.</sZ><sZ>8 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Georges, Patrick" sort="Georges, Patrick" uniqKey="Georges P" first="Patrick" last="Georges">Patrick Georges</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Charles Fabry de l'Institut d'Optique, Université Paris-Sud</s1><s2>91127 Palaiseau</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>7 aut.</sZ><sZ>8 aut.</sZ><sZ>9 aut.</sZ></inist:fA14><country>France</country></affiliation></author><author><name sortKey="Canning, J" sort="Canning, J" uniqKey="Canning J" first="J." last="Canning">J. Canning</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Interdisciplinary Photonics Laboratories, School of Chemistry, University of Sydney</s1><s2>NSW, 2006</s2><s3>AUS</s3><sZ>3 aut.</sZ><sZ>10 aut.</sZ></inist:fA14><country>Australie</country></affiliation></author><author><name sortKey="Buczynski, Ryszard" sort="Buczynski, Ryszard" uniqKey="Buczynski R" first="Ryszard" last="Buczynski">Ryszard Buczynski</name><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Faculty of Physics, University of Warsaw, Pasteura, 7</s1><s2>02-093 Warsaw</s2><s3>POL</s3><sZ>11 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Pysz, Darius" sort="Pysz, Darius" uniqKey="Pysz D" first="Darius" last="Pysz">Darius Pysz</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Glass Laboratory, Institute of Electronic Materials Technology, Wólczyńska, 133</s1><s2>01-919 Warsaw</s2><s3>POL</s3><sZ>12 aut.</sZ><sZ>13 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Stepien, Ryszard" sort="Stepien, Ryszard" uniqKey="Stepien R" first="Ryszard" last="Stepien">Ryszard Stepien</name><affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Glass Laboratory, Institute of Electronic Materials Technology, Wólczyńska, 133</s1><s2>01-919 Warsaw</s2><s3>POL</s3><sZ>12 aut.</sZ><sZ>13 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author></analytic><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="2010">2010</date></imprint></series></biblStruct></sourceDesc><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></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Arsenic sulfides</term><term>Binary compounds</term><term>Bragg gratings</term><term>Chalcogenides</term><term>Diffraction gratings</term><term>Frequency shift</term><term>Gallium</term><term>Glass</term><term>Grating in fiber</term><term>Heavy metal</term><term>Metal oxides</term><term>Microstructured fiber</term><term>Nonlinear optics</term><term>Nonlinear refractive index</term><term>Optical fibers</term><term>Optical frequency conversion</term><term>Optical solitons</term><term>Refractive index</term><term>Silica</term><term>Step index</term><term>Stimulated Raman scattering</term><term>Subpicosecond</term><term>Ultrashort pulse</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Conversion fréquence optique</term><term>Diffusion Raman stimulée</term><term>Soliton optique</term><term>Déplacement fréquence</term><term>Saut indice</term><term>Impulsion ultracourte</term><term>Réseau diffraction</term><term>Réseau dans fibre</term><term>Réseau Bragg</term><term>Optique non linéaire</term><term>Indice réfraction</term><term>Subpicoseconde</term><term>Fibre optique</term><term>Fibre microstructurée</term><term>Composé binaire</term><term>Sulfure d'arsenic</term><term>Silice</term><term>Chalcogénure</term><term>Métal lourd</term><term>Oxyde métallique</term><term>Verre</term><term>Gallium</term><term>As2S3</term><term>As S</term><term>0130C</term><term>4265R</term><term>4281</term><term>4279D</term><term>4265K</term><term>4265D</term><term>4265T</term><term>4281W</term><term>Indice réfraction non linéaire</term></keywords><keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Métal lourd</term><term>Verre</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">Chalcogenide or heavy metal oxide glasses are well known for their good transparency in the mid-infrared (MIR) domain as well as their high nonlinear refractive index (n<sub>2</sub>) tens to hundreds times higher than that of silica. We have investigated the nonlinear frequency conversion processes, based upon either stimulated Raman scattering (SRS) or soliton fission and soliton self-frequency shift (SSFS) in fibres made up with such highly nonlinear infrared transmitting glasses. First, SRS has been investigated in a chalcogenide As<sub>2</sub>S<sub>3</sub> step index fibre. In the single pass configuration, under quasi continuous wave 1550 nm pumping, Raman cascade up to the forth Stokes order has been obtained in a 3 m long piece of fibre. The possibility to build a Raman laser thanks to in-fibre written Bragg gratings has also been investigated. A 5 dB Bragg grating has been written successfully in the core. Then, nonlinear frequency conversion in ultra-short pulse regime has been studied in a heavy metal oxide (lead-bismuth-gallium ternary system) glass photonic crystal fibre. Broadband radiation, from 800 nm up to 2.8 μm, has been obtained by pumping an 8 cm long piece of fibre at 1600 nm in sub-picosecond pulsed regime. The nonlinear frequency conversion process was assessed by numerical modelling taking into account the actual fibre cross-section as well as the measured linear and nonlinear parameters and was found to be due to soliton fission and Raman-induced SSFS.</div></front></TEI><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>7714</s2></fA05><fA08 i1="01" i2="1" l="ENG"><s1>Frequency conversion from near-infrared to mid-infrared in highly nonlinear optical fibres</s1></fA08><fA09 i1="01" i2="1" l="ENG"><s1>Photonic crystal fibers IV : 14-16 April 2010, Brussels, Belgium</s1></fA09><fA11 i1="01" i2="1"><s1>DUCROS (Nicolas)</s1></fA11><fA11 i1="02" i2="1"><s1>MORIN (Franck)</s1></fA11><fA11 i1="03" i2="1"><s1>COOK (Kevin)</s1></fA11><fA11 i1="04" i2="1"><s1>LABRUYERE (Alexis)</s1></fA11><fA11 i1="05" i2="1"><s1>FEVRIER (Sébastien)</s1></fA11><fA11 i1="06" i2="1"><s1>HUMBERT (Georges)</s1></fA11><fA11 i1="07" i2="1"><s1>DRUON (Frédéric)</s1></fA11><fA11 i1="08" i2="1"><s1>HANNA (Marc)</s1></fA11><fA11 i1="09" i2="1"><s1>GEORGES (Patrick)</s1></fA11><fA11 i1="10" i2="1"><s1>CANNING (J.)</s1></fA11><fA11 i1="11" i2="1"><s1>BUCZYNSKI (Ryszard)</s1></fA11><fA11 i1="12" i2="1"><s1>PYSZ (Darius)</s1></fA11><fA11 i1="13" i2="1"><s1>STEPIEN (Ryszard)</s1></fA11><fA12 i1="01" i2="1"><s1>KALLI (Kyriacos)</s1><s9>ed.</s9></fA12><fA12 i1="02" i2="1"><s1>URBA========Nacute;CZYK (Wacław)</s1><s9>ed.</s9></fA12><fA14 i1="01"><s1>Xlim UMR CNRS 6172, 123 avenue A. Thomas</s1><s2>87060 Limoges</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></fA14><fA14 i1="02"><s1>Laboratoire Charles Fabry de l'Institut d'Optique, Université Paris-Sud</s1><s2>91127 Palaiseau</s2><s3>FRA</s3><sZ>2 aut.</sZ><sZ>7 aut.</sZ><sZ>8 aut.</sZ><sZ>9 aut.</sZ></fA14><fA14 i1="03"><s1>Interdisciplinary Photonics Laboratories, School of Chemistry, University of Sydney</s1><s2>NSW, 2006</s2><s3>AUS</s3><sZ>3 aut.</sZ><sZ>10 aut.</sZ></fA14><fA14 i1="04"><s1>Faculty of Physics, University of Warsaw, Pasteura, 7</s1><s2>02-093 Warsaw</s2><s3>POL</s3><sZ>11 aut.</sZ></fA14><fA14 i1="05"><s1>Glass Laboratory, Institute of Electronic Materials Technology, Wólczyńska, 133</s1><s2>01-919 Warsaw</s2><s3>POL</s3><sZ>12 aut.</sZ><sZ>13 aut.</sZ></fA14><fA18 i1="01" i2="1"><s1>SPIE</s1><s3>USA</s3><s9>org-cong.</s9></fA18><fA18 i1="02" i2="1"><s1>B-BHOT--Brussels Photonics Team</s1><s3>BEL</s3><s9>org-cong.</s9></fA18><fA18 i1="03" i2="1"><s1>Comité belge d'optique</s1><s3>BEL</s3><s9>org-cong.</s9></fA18><fA20><s2>77140B.1-77140B.8</s2></fA20><fA21><s1>2010</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA25 i1="01"><s1>SPIE</s1><s2>Bellingham, Wash.</s2></fA25><fA26 i1="01"><s0>0-8194-8187-4</s0></fA26><fA26 i1="02"><s0>978-0-8194-8187-0</s0></fA26><fA43 i1="01"><s1>INIST</s1><s2>21760</s2><s5>354000174704520090</s5></fA43><fA44><s0>0000</s0><s1>© 2011 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>24 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>11-0015340</s0></fA47><fA60><s1>P</s1><s2>C</s2></fA60><fA61><s0>A</s0></fA61><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>Chalcogenide or heavy metal oxide glasses are well known for their good transparency in the mid-infrared (MIR) domain as well as their high nonlinear refractive index (n<sub>2</sub>) tens to hundreds times higher than that of silica. We have investigated the nonlinear frequency conversion processes, based upon either stimulated Raman scattering (SRS) or soliton fission and soliton self-frequency shift (SSFS) in fibres made up with such highly nonlinear infrared transmitting glasses. First, SRS has been investigated in a chalcogenide As<sub>2</sub>S<sub>3</sub> step index fibre. In the single pass configuration, under quasi continuous wave 1550 nm pumping, Raman cascade up to the forth Stokes order has been obtained in a 3 m long piece of fibre. The possibility to build a Raman laser thanks to in-fibre written Bragg gratings has also been investigated. A 5 dB Bragg grating has been written successfully in the core. Then, nonlinear frequency conversion in ultra-short pulse regime has been studied in a heavy metal oxide (lead-bismuth-gallium ternary system) glass photonic crystal fibre. Broadband radiation, from 800 nm up to 2.8 μm, has been obtained by pumping an 8 cm long piece of fibre at 1600 nm in sub-picosecond pulsed regime. The nonlinear frequency conversion process was assessed by numerical modelling taking into account the actual fibre cross-section as well as the measured linear and nonlinear parameters and was found to be due to soliton fission and Raman-induced SSFS.</s0></fC01><fC02 i1="01" i2="3"><s0>001B00A30C</s0></fC02><fC02 i1="02" i2="3"><s0>001B40B65K</s0></fC02><fC02 i1="03" i2="3"><s0>001B40B65D</s0></fC02><fC02 i1="04" i2="3"><s0>001B40B65T</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Conversion fréquence optique</s0><s5>03</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Optical frequency conversion</s0><s5>03</s5></fC03><fC03 i1="02" i2="3" l="FRE"><s0>Diffusion Raman stimulée</s0><s5>04</s5></fC03><fC03 i1="02" i2="3" l="ENG"><s0>Stimulated Raman scattering</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Soliton optique</s0><s5>05</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Optical solitons</s0><s5>05</s5></fC03><fC03 i1="04" i2="X" l="FRE"><s0>Déplacement fréquence</s0><s5>06</s5></fC03><fC03 i1="04" i2="X" l="ENG"><s0>Frequency shift</s0><s5>06</s5></fC03><fC03 i1="04" i2="X" l="SPA"><s0>Desplazamiento frecuencia</s0><s5>06</s5></fC03><fC03 i1="05" i2="X" l="FRE"><s0>Saut indice</s0><s5>07</s5></fC03><fC03 i1="05" i2="X" l="ENG"><s0>Step index</s0><s5>07</s5></fC03><fC03 i1="05" i2="X" l="SPA"><s0>Salto indicativo</s0><s5>07</s5></fC03><fC03 i1="06" i2="X" l="FRE"><s0>Impulsion ultracourte</s0><s5>08</s5></fC03><fC03 i1="06" i2="X" l="ENG"><s0>Ultrashort pulse</s0><s5>08</s5></fC03><fC03 i1="06" i2="X" l="SPA"><s0>Impulsión ultracorto</s0><s5>08</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Réseau diffraction</s0><s5>09</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Diffraction gratings</s0><s5>09</s5></fC03><fC03 i1="08" i2="X" l="FRE"><s0>Réseau dans fibre</s0><s5>11</s5></fC03><fC03 i1="08" i2="X" l="ENG"><s0>Grating in fiber</s0><s5>11</s5></fC03><fC03 i1="08" i2="X" l="SPA"><s0>Red en fibra</s0><s5>11</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Réseau Bragg</s0><s5>12</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Bragg gratings</s0><s5>12</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Optique non linéaire</s0><s5>17</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Nonlinear optics</s0><s5>17</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Indice réfraction</s0><s5>41</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Refractive index</s0><s5>41</s5></fC03><fC03 i1="12" i2="X" l="FRE"><s0>Subpicoseconde</s0><s5>42</s5></fC03><fC03 i1="12" i2="X" l="ENG"><s0>Subpicosecond</s0><s5>42</s5></fC03><fC03 i1="12" i2="X" l="SPA"><s0>Subpicosegundo</s0><s5>42</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>Fibre microstructurée</s0><s5>48</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Microstructured fiber</s0><s5>48</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Composé binaire</s0><s5>50</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>Binary compounds</s0><s5>50</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Sulfure d'arsenic</s0><s2>NK</s2><s5>51</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Arsenic sulfides</s0><s2>NK</s2><s5>51</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Silice</s0><s2>NK</s2><s5>57</s5></fC03><fC03 i1="17" i2="3" l="ENG"><s0>Silica</s0><s2>NK</s2><s5>57</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>Chalcogénure</s0><s2>NA</s2><s5>61</s5></fC03><fC03 i1="18" i2="3" l="ENG"><s0>Chalcogenides</s0><s2>NA</s2><s5>61</s5></fC03><fC03 i1="19" i2="X" l="FRE"><s0>Métal lourd</s0><s5>62</s5></fC03><fC03 i1="19" i2="X" l="ENG"><s0>Heavy metal</s0><s5>62</s5></fC03><fC03 i1="19" i2="X" l="SPA"><s0>Metal pesado</s0><s5>62</s5></fC03><fC03 i1="20" i2="3" l="FRE"><s0>Oxyde métallique</s0><s5>63</s5></fC03><fC03 i1="20" i2="3" l="ENG"><s0>Metal oxides</s0><s5>63</s5></fC03><fC03 i1="21" i2="3" l="FRE"><s0>Verre</s0><s5>64</s5></fC03><fC03 i1="21" i2="3" l="ENG"><s0>Glass</s0><s5>64</s5></fC03><fC03 i1="22" i2="3" l="FRE"><s0>Gallium</s0><s2>NC</s2><s5>65</s5></fC03><fC03 i1="22" i2="3" l="ENG"><s0>Gallium</s0><s2>NC</s2><s5>65</s5></fC03><fC03 i1="23" i2="3" l="FRE"><s0>As2S3</s0><s4>INC</s4><s5>71</s5></fC03><fC03 i1="24" i2="3" l="FRE"><s0>As S</s0><s4>INC</s4><s5>75</s5></fC03><fC03 i1="25" i2="3" l="FRE"><s0>0130C</s0><s4>INC</s4><s5>83</s5></fC03><fC03 i1="26" i2="3" l="FRE"><s0>4265R</s0><s4>INC</s4><s5>84</s5></fC03><fC03 i1="27" i2="3" l="FRE"><s0>4281</s0><s4>INC</s4><s5>85</s5></fC03><fC03 i1="28" i2="3" l="FRE"><s0>4279D</s0><s4>INC</s4><s5>86</s5></fC03><fC03 i1="29" i2="3" l="FRE"><s0>4265K</s0><s4>INC</s4><s5>91</s5></fC03><fC03 i1="30" i2="3" l="FRE"><s0>4265D</s0><s4>INC</s4><s5>92</s5></fC03><fC03 i1="31" i2="3" l="FRE"><s0>4265T</s0><s4>INC</s4><s5>93</s5></fC03><fC03 i1="32" i2="3" l="FRE"><s0>4281W</s0><s4>INC</s4><s5>94</s5></fC03><fC03 i1="33" i2="3" l="FRE"><s0>Indice réfraction non linéaire</s0><s4>CD</s4><s5>96</s5></fC03><fC03 i1="33" i2="3" l="ENG"><s0>Nonlinear refractive index</s0><s4>CD</s4><s5>96</s5></fC03><fC07 i1="01" i2="3" l="FRE"><s0>Diffusion stimulée</s0></fC07><fC07 i1="01" i2="3" l="ENG"><s0>Stimulated scattering</s0></fC07><fN21><s1>003</s1></fN21><fN44 i1="01"><s1>OTO</s1></fN44><fN82><s1>OTO</s1></fN82></pA><pR><fA30 i1="01" i2="1" l="ENG"><s1>Photonic crystal fibers</s1><s2>04</s2><s3>Brussels BEL</s3><s4>2010</s4></fA30></pR></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
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