Fiber lasers : new effective sources for coherent lidars
Identifieur interne :
000620 ( Pascal/Curation );
précédent :
000619;
suivant :
000621
Fiber lasers : new effective sources for coherent lidars
Auteurs : Jean-Pierre Cariou [
France] ;
Matthieu Valla [
France] ;
Guillaume Canat [
France]
Source :
-
Proceedings of SPIE - The International Society for Optical Engineering [ 0277-786X ] ; 2007.
RBID : Pascal:08-0383673
Descripteurs français
- Pascal (Inist)
- Communication fibre optique,
Effet non linéaire,
Lidar,
Télécommunication optique,
Télédétection,
Fibre optique,
Fibre double gaine,
Fibre monomode,
Ytterbium,
Thulium,
Oeil,
Méthode mesure,
Méthode optique,
Optique atmosphérique,
0130C,
4268W,
4279S.
- Wicri :
English descriptors
- KwdEn :
- Atmospheric optics,
Doubly clad fiber,
Eyes,
Lidar,
Measuring methods,
Non linear effect,
Optical communication,
Optical fiber communication,
Optical fibers,
Optical method,
Remote sensing,
Single mode fiber,
Thulium,
Ytterbium.
Abstract
Originally developed for telecommunications, fiber lasers are now becoming new effective sources for coherent lidars allowing new instruments to be designed. The advent of the double clad fiber, along with advances in semiconductor pump diode sources, have allowed rapid power scaling of both pulsed and CW fiber sources. The unique capabilities of fiber sources, coupled with significant commercial and academic progress in implementation, have driven fiber technology to enter active remote sensing markets as signal sources and amplification stages for direct detection lidars and coherent lidars as well. Some interesting fiber lasers benefit from a good transmission in the near infrared spectral band: Ytterbium lasers (1.0-1.06μm), Erbium lasers (1.48-1.62μm) and Thulium lasers (1.8-2.1μm). However, useful wavelengths have to be tuned between absorption H20 and C02 lines. Eye safety may be an issue for atmospheric lidars. Above 1.4 μm, the maximum permitted exposure (MPE) is 3 orders of magnitude higher than for shorter wavelengths and an eye-safe operation is possible even with multi-watt lasers. Low power fiber lasers using single mode fibers have a good spatial quality. However, higher power lasers and amplifiers need larger fiber cores, to store enough energy and to avoid non linear effects. Trade-off between high power, single mode operation, stable polarization and spectral quality need to be considered for coherent lidars.
| pA |
| A01 | 01 | 1 | | @0 0277-786X |
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| A05 | | | | @2 6750 |
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| A08 | 01 | 1 | ENG | @1 Fiber lasers : new effective sources for coherent lidars |
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| A09 | 01 | 1 | ENG | @1 Lidar technologies, techniques, and measurements for atmospheric remote sensing III : 17 September 2007, Florence, Italy |
|---|
| A11 | 01 | 1 | | @1 CARIOU (Jean-Pierre) |
|---|
| A11 | 02 | 1 | | @1 VALLA (Matthieu) |
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| A11 | 03 | 1 | | @1 CANAT (Guillaume) |
|---|
| A12 | 01 | 1 | | @1 SINGH (Upendra N.) @9 ed. |
|---|
| A12 | 02 | 1 | | @1 PAPPALARDO (Gelsomina) @9 ed. |
|---|
| A14 | 01 | | | @1 LEOSPHERE, Bat 503, Centre Scientifique d'Orsay @2 91400 Orsay @3 FRA @Z 1 aut. |
|---|
| A14 | 02 | | | @1 ONERA/DOTA, Chemin de la Hunière @2 91761 Palaiseau @3 FRA @Z 2 aut. @Z 3 aut. |
|---|
| A18 | 01 | 1 | | @1 SPIE @3 USA @9 org-cong. |
|---|
| A20 | | | | @2 675007.1-675007.12 |
|---|
| A21 | | | | @1 2007 |
|---|
| A23 | 01 | | | @0 ENG |
|---|
| A26 | 01 | | | @0 978-0-8194-6908-3 |
|---|
| A43 | 01 | | | @1 INIST @2 21760 @5 354000172837310050 |
|---|
| A44 | | | | @0 0000 @1 © 2008 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 22 ref. |
|---|
| A47 | 01 | 1 | | @0 08-0383673 |
|---|
| A60 | | | | @1 P @2 C |
|---|
| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 Proceedings of SPIE - The International Society for Optical Engineering |
|---|
| A66 | 01 | | | @0 USA |
|---|
| C01 | 01 | | ENG | @0 Originally developed for telecommunications, fiber lasers are now becoming new effective sources for coherent lidars allowing new instruments to be designed. The advent of the double clad fiber, along with advances in semiconductor pump diode sources, have allowed rapid power scaling of both pulsed and CW fiber sources. The unique capabilities of fiber sources, coupled with significant commercial and academic progress in implementation, have driven fiber technology to enter active remote sensing markets as signal sources and amplification stages for direct detection lidars and coherent lidars as well. Some interesting fiber lasers benefit from a good transmission in the near infrared spectral band: Ytterbium lasers (1.0-1.06μm), Erbium lasers (1.48-1.62μm) and Thulium lasers (1.8-2.1μm). However, useful wavelengths have to be tuned between absorption H20 and C02 lines. Eye safety may be an issue for atmospheric lidars. Above 1.4 μm, the maximum permitted exposure (MPE) is 3 orders of magnitude higher than for shorter wavelengths and an eye-safe operation is possible even with multi-watt lasers. Low power fiber lasers using single mode fibers have a good spatial quality. However, higher power lasers and amplifiers need larger fiber cores, to store enough energy and to avoid non linear effects. Trade-off between high power, single mode operation, stable polarization and spectral quality need to be considered for coherent lidars. |
|---|
| C02 | 01 | 3 | | @0 001B00A30C |
|---|
| C02 | 02 | 3 | | @0 001B40B68W |
|---|
| C02 | 03 | X | | @0 001D04B08 |
|---|
| C03 | 01 | 3 | FRE | @0 Communication fibre optique @5 03 |
|---|
| C03 | 01 | 3 | ENG | @0 Optical fiber communication @5 03 |
|---|
| C03 | 02 | X | FRE | @0 Effet non linéaire @5 04 |
|---|
| C03 | 02 | X | ENG | @0 Non linear effect @5 04 |
|---|
| C03 | 02 | X | SPA | @0 Efecto no lineal @5 04 |
|---|
| C03 | 03 | 3 | FRE | @0 Lidar @5 11 |
|---|
| C03 | 03 | 3 | ENG | @0 Lidar @5 11 |
|---|
| C03 | 04 | 3 | FRE | @0 Télécommunication optique @5 17 |
|---|
| C03 | 04 | 3 | ENG | @0 Optical communication @5 17 |
|---|
| C03 | 05 | 3 | FRE | @0 Télédétection @5 30 |
|---|
| C03 | 05 | 3 | ENG | @0 Remote sensing @5 30 |
|---|
| C03 | 06 | 3 | FRE | @0 Fibre optique @5 47 |
|---|
| C03 | 06 | 3 | ENG | @0 Optical fibers @5 47 |
|---|
| C03 | 07 | X | FRE | @0 Fibre double gaine @5 48 |
|---|
| C03 | 07 | X | ENG | @0 Doubly clad fiber @5 48 |
|---|
| C03 | 07 | X | SPA | @0 Fibra chapado doble @5 48 |
|---|
| C03 | 08 | X | FRE | @0 Fibre monomode @5 49 |
|---|
| C03 | 08 | X | ENG | @0 Single mode fiber @5 49 |
|---|
| C03 | 08 | X | SPA | @0 Fibra monomoda @5 49 |
|---|
| C03 | 09 | 3 | FRE | @0 Ytterbium @2 NC @5 61 |
|---|
| C03 | 09 | 3 | ENG | @0 Ytterbium @2 NC @5 61 |
|---|
| C03 | 10 | 3 | FRE | @0 Thulium @2 NC @5 62 |
|---|
| C03 | 10 | 3 | ENG | @0 Thulium @2 NC @5 62 |
|---|
| C03 | 11 | 3 | FRE | @0 Oeil @5 63 |
|---|
| C03 | 11 | 3 | ENG | @0 Eyes @5 63 |
|---|
| C03 | 12 | 3 | FRE | @0 Méthode mesure @5 64 |
|---|
| C03 | 12 | 3 | ENG | @0 Measuring methods @5 64 |
|---|
| C03 | 13 | X | FRE | @0 Méthode optique @5 65 |
|---|
| C03 | 13 | X | ENG | @0 Optical method @5 65 |
|---|
| C03 | 13 | X | SPA | @0 Método óptico @5 65 |
|---|
| C03 | 14 | 3 | FRE | @0 Optique atmosphérique @5 66 |
|---|
| C03 | 14 | 3 | ENG | @0 Atmospheric optics @5 66 |
|---|
| C03 | 15 | 3 | FRE | @0 0130C @4 INC @5 83 |
|---|
| C03 | 16 | 3 | FRE | @0 4268W @4 INC @5 84 |
|---|
| C03 | 17 | 3 | FRE | @0 4279S @4 INC @5 91 |
|---|
| N21 | | | | @1 245 |
|---|
| N44 | 01 | | | @1 OTO |
|---|
| N82 | | | | @1 OTO |
|---|
|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 Lidar technologies, techniques, and measurements for atmospheric remote sensing @2 3 @3 Florence ITA @4 2007 |
|---|
|
|---|
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Le document en format XML
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<author><name sortKey="Cariou, Jean Pierre" sort="Cariou, Jean Pierre" uniqKey="Cariou J" first="Jean-Pierre" last="Cariou">Jean-Pierre Cariou</name>
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<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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</affiliation><series><title level="j" type="main">Proceedings of SPIE - The International Society for Optical Engineering</title>
<idno type="ISSN">0277-786X</idno>
<imprint><date when="2007">2007</date>
</imprint><seriesStmt><title level="j" type="main">Proceedings of SPIE - The International Society for Optical Engineering</title>
<idno type="ISSN">0277-786X</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Atmospheric optics</term>
<term>Doubly clad fiber</term>
<term>Eyes</term>
<term>Lidar</term>
<term>Measuring methods</term>
<term>Non linear effect</term>
<term>Optical communication</term>
<term>Optical fiber communication</term>
<term>Optical fibers</term>
<term>Optical method</term>
<term>Remote sensing</term>
<term>Single mode fiber</term>
<term>Thulium</term>
<term>Ytterbium</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Communication fibre optique</term>
<term>Effet non linéaire</term>
<term>Lidar</term>
<term>Télécommunication optique</term>
<term>Télédétection</term>
<term>Fibre optique</term>
<term>Fibre double gaine</term>
<term>Fibre monomode</term>
<term>Ytterbium</term>
<term>Thulium</term>
<term>Oeil</term>
<term>Méthode mesure</term>
<term>Méthode optique</term>
<term>Optique atmosphérique</term>
<term>0130C</term>
<term>4268W</term>
<term>4279S</term>
</keywords><keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Télédétection</term>
</keywords><front><div type="abstract" xml:lang="en">Originally developed for telecommunications, fiber lasers are now becoming new effective sources for coherent lidars allowing new instruments to be designed. The advent of the double clad fiber, along with advances in semiconductor pump diode sources, have allowed rapid power scaling of both pulsed and CW fiber sources. The unique capabilities of fiber sources, coupled with significant commercial and academic progress in implementation, have driven fiber technology to enter active remote sensing markets as signal sources and amplification stages for direct detection lidars and coherent lidars as well. Some interesting fiber lasers benefit from a good transmission in the near infrared spectral band: Ytterbium lasers (1.0-1.06μm), Erbium lasers (1.48-1.62μm) and Thulium lasers (1.8-2.1μm). However, useful wavelengths have to be tuned between absorption H20 and C02 lines. Eye safety may be an issue for atmospheric lidars. Above 1.4 μm, the maximum permitted exposure (MPE) is 3 orders of magnitude higher than for shorter wavelengths and an eye-safe operation is possible even with multi-watt lasers. Low power fiber lasers using single mode fibers have a good spatial quality. However, higher power lasers and amplifiers need larger fiber cores, to store enough energy and to avoid non linear effects. Trade-off between high power, single mode operation, stable polarization and spectral quality need to be considered for coherent lidars.</div>
</front><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0277-786X</s0>
</fA01><fA05><s2>6750</s2>
</fA05><fA08 i1="01" i2="1" l="ENG"><s1>Fiber lasers : new effective sources for coherent lidars</s1>
</fA08><fA09 i1="01" i2="1" l="ENG"><s1>Lidar technologies, techniques, and measurements for atmospheric remote sensing III : 17 September 2007, Florence, Italy</s1>
</fA09><fA11 i1="01" i2="1"><s1>CARIOU (Jean-Pierre)</s1>
</fA11><fA11 i1="02" i2="1"><s1>VALLA (Matthieu)</s1>
</fA11><fA11 i1="03" i2="1"><s1>CANAT (Guillaume)</s1>
</fA11><fA12 i1="01" i2="1"><s1>SINGH (Upendra N.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="02" i2="1"><s1>PAPPALARDO (Gelsomina)</s1>
<s9>ed.</s9>
</fA12><fA14 i1="01"><s1>LEOSPHERE, Bat 503, Centre Scientifique d'Orsay</s1>
<s2>91400 Orsay</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
</fA14><fA14 i1="02"><s1>ONERA/DOTA, Chemin de la Hunière</s1>
<s2>91761 Palaiseau</s2>
<s3>FRA</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14><fA18 i1="01" i2="1"><s1>SPIE</s1>
<s3>USA</s3>
<s9>org-cong.</s9>
</fA18><fA20><s2>675007.1-675007.12</s2>
</fA20><fA21><s1>2007</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA26 i1="01"><s0>978-0-8194-6908-3</s0>
</fA26><fA43 i1="01"><s1>INIST</s1>
<s2>21760</s2>
<s5>354000172837310050</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2008 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>22 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>08-0383673</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>Originally developed for telecommunications, fiber lasers are now becoming new effective sources for coherent lidars allowing new instruments to be designed. The advent of the double clad fiber, along with advances in semiconductor pump diode sources, have allowed rapid power scaling of both pulsed and CW fiber sources. The unique capabilities of fiber sources, coupled with significant commercial and academic progress in implementation, have driven fiber technology to enter active remote sensing markets as signal sources and amplification stages for direct detection lidars and coherent lidars as well. Some interesting fiber lasers benefit from a good transmission in the near infrared spectral band: Ytterbium lasers (1.0-1.06μm), Erbium lasers (1.48-1.62μm) and Thulium lasers (1.8-2.1μm). However, useful wavelengths have to be tuned between absorption H20 and C02 lines. Eye safety may be an issue for atmospheric lidars. Above 1.4 μm, the maximum permitted exposure (MPE) is 3 orders of magnitude higher than for shorter wavelengths and an eye-safe operation is possible even with multi-watt lasers. Low power fiber lasers using single mode fibers have a good spatial quality. However, higher power lasers and amplifiers need larger fiber cores, to store enough energy and to avoid non linear effects. Trade-off between high power, single mode operation, stable polarization and spectral quality need to be considered for coherent lidars.</s0>
</fC01><fC02 i1="01" i2="3"><s0>001B00A30C</s0>
</fC02><fC02 i1="02" i2="3"><s0>001B40B68W</s0>
</fC02><fC02 i1="03" i2="X"><s0>001D04B08</s0>
</fC02><fC03 i1="01" i2="3" l="FRE"><s0>Communication fibre optique</s0>
<s5>03</s5>
</fC03><fC03 i1="01" i2="3" l="ENG"><s0>Optical fiber communication</s0>
<s5>03</s5>
</fC03><fC03 i1="02" i2="X" l="FRE"><s0>Effet non linéaire</s0>
<s5>04</s5>
</fC03><fC03 i1="02" i2="X" l="ENG"><s0>Non linear effect</s0>
<s5>04</s5>
</fC03><fC03 i1="02" i2="X" l="SPA"><s0>Efecto no lineal</s0>
<s5>04</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Lidar</s0>
<s5>11</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>Lidar</s0>
<s5>11</s5>
</fC03><fC03 i1="04" i2="3" l="FRE"><s0>Télécommunication optique</s0>
<s5>17</s5>
</fC03><fC03 i1="04" i2="3" l="ENG"><s0>Optical communication</s0>
<s5>17</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Télédétection</s0>
<s5>30</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Remote sensing</s0>
<s5>30</s5>
</fC03><fC03 i1="06" i2="3" l="FRE"><s0>Fibre optique</s0>
<s5>47</s5>
</fC03><fC03 i1="06" i2="3" l="ENG"><s0>Optical fibers</s0>
<s5>47</s5>
</fC03><fC03 i1="07" i2="X" l="FRE"><s0>Fibre double gaine</s0>
<s5>48</s5>
</fC03><fC03 i1="07" i2="X" l="ENG"><s0>Doubly clad fiber</s0>
<s5>48</s5>
</fC03><fC03 i1="07" i2="X" l="SPA"><s0>Fibra chapado doble</s0>
<s5>48</s5>
</fC03><fC03 i1="08" i2="X" l="FRE"><s0>Fibre monomode</s0>
<s5>49</s5>
</fC03><fC03 i1="08" i2="X" l="ENG"><s0>Single mode fiber</s0>
<s5>49</s5>
</fC03><fC03 i1="08" i2="X" l="SPA"><s0>Fibra monomoda</s0>
<s5>49</s5>
</fC03><fC03 i1="09" i2="3" l="FRE"><s0>Ytterbium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="09" i2="3" l="ENG"><s0>Ytterbium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03><fC03 i1="10" i2="3" l="FRE"><s0>Thulium</s0>
<s2>NC</s2>
<s5>62</s5>
</fC03><fC03 i1="10" i2="3" l="ENG"><s0>Thulium</s0>
<s2>NC</s2>
<s5>62</s5>
</fC03><fC03 i1="11" i2="3" l="FRE"><s0>Oeil</s0>
<s5>63</s5>
</fC03><fC03 i1="11" i2="3" l="ENG"><s0>Eyes</s0>
<s5>63</s5>
</fC03><fC03 i1="12" i2="3" l="FRE"><s0>Méthode mesure</s0>
<s5>64</s5>
</fC03><fC03 i1="12" i2="3" l="ENG"><s0>Measuring methods</s0>
<s5>64</s5>
</fC03><fC03 i1="13" i2="X" l="FRE"><s0>Méthode optique</s0>
<s5>65</s5>
</fC03><fC03 i1="13" i2="X" l="ENG"><s0>Optical method</s0>
<s5>65</s5>
</fC03><fC03 i1="13" i2="X" l="SPA"><s0>Método óptico</s0>
<s5>65</s5>
</fC03><fC03 i1="14" i2="3" l="FRE"><s0>Optique atmosphérique</s0>
<s5>66</s5>
</fC03><fC03 i1="14" i2="3" l="ENG"><s0>Atmospheric optics</s0>
<s5>66</s5>
</fC03><fC03 i1="15" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03><fC03 i1="16" i2="3" l="FRE"><s0>4268W</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03><fC03 i1="17" i2="3" l="FRE"><s0>4279S</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03><fN21><s1>245</s1>
</fN21><fN44 i1="01"><s1>OTO</s1>
</fN44><fN82><s1>OTO</s1>
</fN82><pR><fA30 i1="01" i2="1" l="ENG"><s1>Lidar technologies, techniques, and measurements for atmospheric remote sensing</s1>
<s2>3</s2>
<s3>Florence ITA</s3>
<s4>2007</s4>
</fA30>
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