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Rediscovered dynamics of nonlinear fiber optics -from breathers to extreme localisation

Identifieur interne : 004484 ( PascalFrancis/Curation ); précédent : 004483; suivant : 004485

Rediscovered dynamics of nonlinear fiber optics -from breathers to extreme localisation

Auteurs : Bertrand Kibler [France] ; Julien Fatome [France] ; Christophe Finot [France] ; Kamal Hammani [France] ; Guy Millot [France] ; Frederic Dias [Irlande (pays)] ; Goery Genty [Finlande] ; Miro Erkintalo [Finlande] ; Nail Akhmediev [Australie] ; Benjamin Wetzel [France] ; John M. Dudley [France]

Source :

RBID : Pascal:11-0357769

Descripteurs français

English descriptors

Abstract

Recent investigations in nonlinear fiber optics have shown a renewed interest in certain classes of analytical solutions of the Nonlinear Schrödinger equation which, although present in the mathematical literature for 25 years, have been largely overlooked in studies of nonlinear fiber propagation. In this paper we review recent experiments that have shown the power of this analytic approach.
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A30 01  1  ENG  @1 Nonlinear frequency generation and conversion @2 10 @3 San Francisco CA USA @4 2011

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Pascal:11-0357769

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<s1>Laboratoire Interdisciplinaire Carnot de Bourgogne, UMR 5209 CNRS - Université de Bourgogne</s1>
<s2>Dijon</s2>
<s3>FRA</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>Centre de Mathématiques et de Leurs Applications (CMLA), ENS Cachan, France ; UCD School of Mathematical Sciences, University College Dublin</s1>
<s2>Belfield, Dublin</s2>
<s3>IRL</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="03">
<s1>Tampere University of Technology, Optics Laboratory</s1>
<s2>33101 Tampere</s2>
<s3>FIN</s3>
<sZ>7 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="04">
<s1>Optical Sciences Group, Research School of Physics and Engineering, Institute of Advanced Studies, The Australian National University</s1>
<s2>Canberra ACT 0200</s2>
<s3>AUS</s3>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="05">
<s1>Institut FEMTO-ST, UMR 6174 CNRS- Université de Franche-Comté</s1>
<s2>25030 Besançon</s2>
<s3>FRA</s3>
<sZ>10 aut.</sZ>
<sZ>11 aut.</sZ>
</fA14>
<fA18 i1="01" i2="1">
<s1>SPIE</s1>
<s3>USA</s3>
<s9>org-cong.</s9>
</fA18>
<fA20>
<s2>79170W.1-79170W.6</s2>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA25 i1="01">
<s1>SPIE</s1>
<s2>Bellingham, Wash.</s2>
</fA25>
<fA26 i1="01">
<s0>978-0-8194-8454-3</s0>
</fA26>
<fA43 i1="01">
<s1>INIST</s1>
<s2>21760</s2>
<s5>354000174738370290</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>16 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0357769</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>Recent investigations in nonlinear fiber optics have shown a renewed interest in certain classes of analytical solutions of the Nonlinear Schrödinger equation which, although present in the mathematical literature for 25 years, have been largely overlooked in studies of nonlinear fiber propagation. In this paper we review recent experiments that have shown the power of this analytic approach.</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>001B40B65R</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Optique non linéaire</s0>
<s5>19</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Nonlinear optics</s0>
<s5>19</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Etude théorique</s0>
<s5>21</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Theoretical study</s0>
<s5>21</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Solution analytique</s0>
<s5>23</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Analytical solution</s0>
<s5>23</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Equation non linéaire</s0>
<s5>24</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Nonlinear equations</s0>
<s5>24</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Equation Schrödinger</s0>
<s5>25</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Schroedinger equation</s0>
<s5>25</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Méthode analytique</s0>
<s5>26</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Analytical method</s0>
<s5>26</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Método analítico</s0>
<s5>26</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Optique ultrarapide</s0>
<s5>61</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Ultrafast optics</s0>
<s5>61</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>4265K</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>4265R</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fN21>
<s1>249</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
<pR>
<fA30 i1="01" i2="1" l="ENG">
<s1>Nonlinear frequency generation and conversion</s1>
<s2>10</s2>
<s3>San Francisco CA USA</s3>
<s4>2011</s4>
</fA30>
</pR>
</standard>
</inist>
</record>

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