Generation and Amplification of femtosecond pulses in Tm:fiber
Identifieur interne :
000187 ( Pascal/Corpus );
précédent :
000186;
suivant :
000188
Generation and Amplification of femtosecond pulses in Tm:fiber
Auteurs : R. Andrew Sims ;
Pankaj Kadwani ;
Lawrence Shah ;
Martin RichardsonSource :
-
Proceedings of SPIE, the International Society for Optical Engineering [ 0277-786X ] ; 2011.
RBID : Pascal:12-0011745
Descripteurs français
- Pascal (Inist)
- Soliton optique,
Amplificateur optique,
Résonateur anneau,
Optique non linéaire,
Application laser,
Domaine temps fs,
Durée impulsion,
Application militaire,
0130C,
4262,
4265T,
8920D,
4260D,
Fibre dopée thulium,
Amplificateur Raman.
English descriptors
Abstract
We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
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 Generation and Amplification of femtosecond pulses in Tm:fiber |
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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 SIMS (R. Andrew) |
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A11 | 02 | 1 | | @1 KADWANI (Pankaj) |
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A11 | 03 | 1 | | @1 SHAH (Lawrence) |
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A11 | 04 | 1 | | @1 RICHARDSON (Martin) |
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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. |
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A18 | 01 | 1 | | @1 SPIE @3 USA @9 org-cong. |
---|
A20 | | | | @2 80390K.1-80390K.4 |
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A21 | | | | @1 2011 |
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A23 | 01 | | | @0 ENG |
---|
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 354000174755190120 |
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A44 | | | | @0 0000 @1 © 2012 INIST-CNRS. All rights reserved. |
---|
A45 | | | | @0 8 ref. |
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A47 | 01 | 1 | | @0 12-0011745 |
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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 |
---|
A66 | 01 | | | @0 USA |
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C01 | 01 | | ENG | @0 We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs. |
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C02 | 01 | 3 | | @0 001B00A30C |
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C02 | 02 | 3 | | @0 001B40B62 |
---|
C02 | 03 | 3 | | @0 001B40B65T |
---|
C02 | 04 | X | | @0 001D17 |
---|
C03 | 01 | 3 | FRE | @0 Soliton optique @5 03 |
---|
C03 | 01 | 3 | ENG | @0 Optical solitons @5 03 |
---|
C03 | 02 | X | FRE | @0 Amplificateur optique @5 09 |
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C03 | 02 | X | ENG | @0 Optical amplifier @5 09 |
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C03 | 02 | X | SPA | @0 Amplificador óptico @5 09 |
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C03 | 03 | X | FRE | @0 Résonateur anneau @5 11 |
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C03 | 03 | X | ENG | @0 Ring resonator @5 11 |
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C03 | 03 | X | SPA | @0 Resonador anillo @5 11 |
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C03 | 04 | 3 | FRE | @0 Optique non linéaire @5 17 |
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C03 | 04 | 3 | ENG | @0 Nonlinear optics @5 17 |
---|
C03 | 05 | 3 | FRE | @0 Application laser @5 19 |
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C03 | 05 | 3 | ENG | @0 Laser beam applications @5 19 |
---|
C03 | 06 | 3 | FRE | @0 Domaine temps fs @5 41 |
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C03 | 06 | 3 | ENG | @0 fs range @5 41 |
---|
C03 | 07 | X | FRE | @0 Durée impulsion @5 42 |
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C03 | 07 | X | ENG | @0 Pulse width @5 42 |
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C03 | 07 | X | SPA | @0 Duración impulso @5 42 |
---|
C03 | 08 | X | FRE | @0 Application militaire @5 61 |
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C03 | 08 | X | ENG | @0 Military application @5 61 |
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C03 | 08 | X | SPA | @0 Aplicación militar @5 61 |
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C03 | 09 | 3 | FRE | @0 0130C @4 INC @5 83 |
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C03 | 10 | 3 | FRE | @0 4262 @4 INC @5 84 |
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C03 | 11 | 3 | FRE | @0 4265T @4 INC @5 91 |
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C03 | 12 | 3 | FRE | @0 8920D @4 INC @5 92 |
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C03 | 13 | 3 | FRE | @0 4260D @4 INC @5 93 |
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C03 | 14 | 3 | FRE | @0 Fibre dopée thulium @4 CD @5 96 |
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C03 | 14 | 3 | ENG | @0 Thulium-doped fibers @4 CD @5 96 |
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C03 | 15 | 3 | FRE | @0 Amplificateur Raman @4 CD @5 97 |
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C03 | 15 | 3 | ENG | @0 Raman amplifier @4 CD @5 97 |
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N21 | | | | @1 002 |
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N44 | 01 | | | @1 OTO |
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N82 | | | | @1 OTO |
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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 |
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|
Format Inist (serveur)
NO : | PASCAL 12-0011745 INIST |
ET : | Generation and Amplification of femtosecond pulses in Tm:fiber |
AU : | SIMS (R. Andrew); KADWANI (Pankaj); SHAH (Lawrence); RICHARDSON (Martin); DUBINSKII (Mark A.); POST (Stephen G.) |
AF : | Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard/Orlando, Florida 32816/Etats-Unis (1 aut., 2 aut., 3 aut., 4 aut.) |
DT : | Publication en série; Congrès; Niveau analytique |
SO : | Proceedings of SPIE, the International Society for Optical Engineering; ISSN 0277-786X; Coden PSISDG; Etats-Unis; Da. 2011; Vol. 8039; 80390K.1-80390K.4; Bibl. 8 ref. |
LA : | Anglais |
EA : | We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs. |
CC : | 001B00A30C; 001B40B62; 001B40B65T; 001D17 |
FD : | Soliton optique; Amplificateur optique; Résonateur anneau; Optique non linéaire; Application laser; Domaine temps fs; Durée impulsion; Application militaire; 0130C; 4262; 4265T; 8920D; 4260D; Fibre dopée thulium; Amplificateur Raman |
ED : | Optical solitons; Optical amplifier; Ring resonator; Nonlinear optics; Laser beam applications; fs range; Pulse width; Military application; Thulium-doped fibers; Raman amplifier |
SD : | Amplificador óptico; Resonador anillo; Duración impulso; Aplicación militar |
LO : | INIST-21760.354000174755190120 |
ID : | 12-0011745 |
Links to Exploration step
Pascal:12-0011745
Le document en format XML
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<front><div type="abstract" xml:lang="en">We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs.</div>
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<fC01 i1="01" l="ENG"><s0>We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs.</s0>
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<s5>03</s5>
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<s5>09</s5>
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<s5>09</s5>
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<s5>09</s5>
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<s5>11</s5>
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<s5>11</s5>
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<s5>11</s5>
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<s5>17</s5>
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<s5>17</s5>
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<s5>41</s5>
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<s5>41</s5>
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<fC03 i1="07" i2="X" l="FRE"><s0>Durée impulsion</s0>
<s5>42</s5>
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<s5>42</s5>
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<s5>42</s5>
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<s5>61</s5>
</fC03>
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<s5>61</s5>
</fC03>
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<s5>61</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
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<s5>84</s5>
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<s4>INC</s4>
<s5>91</s5>
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<fC03 i1="12" i2="3" l="FRE"><s0>8920D</s0>
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<s5>92</s5>
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<fC03 i1="13" i2="3" l="FRE"><s0>4260D</s0>
<s4>INC</s4>
<s5>93</s5>
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<fC03 i1="14" i2="3" l="FRE"><s0>Fibre dopée thulium</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Thulium-doped fibers</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Amplificateur Raman</s0>
<s4>CD</s4>
<s5>97</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Raman amplifier</s0>
<s4>CD</s4>
<s5>97</s5>
</fC03>
<fN21><s1>002</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
<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>
</pR>
</standard>
<server><NO>PASCAL 12-0011745 INIST</NO>
<ET>Generation and Amplification of femtosecond pulses in Tm:fiber</ET>
<AU>SIMS (R. Andrew); KADWANI (Pankaj); SHAH (Lawrence); RICHARDSON (Martin); DUBINSKII (Mark A.); POST (Stephen G.)</AU>
<AF>Townes Laser Institute, CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Boulevard/Orlando, Florida 32816/Etats-Unis (1 aut., 2 aut., 3 aut., 4 aut.)</AF>
<DT>Publication en série; Congrès; Niveau analytique</DT>
<SO>Proceedings of SPIE, the International Society for Optical Engineering; ISSN 0277-786X; Coden PSISDG; Etats-Unis; Da. 2011; Vol. 8039; 80390K.1-80390K.4; Bibl. 8 ref.</SO>
<LA>Anglais</LA>
<EA>We describe the generation and amplification of femtosecond pulses at 2-μm wavelength in thulium doped fiber. The mode-locked oscillator is a ring cavity based on single-mode Tm:fiber producing stable soliton pulses at 70 MHz repetition rate with 40 pJ pulse energy, centered at ∼1.97 μm wavelength with ∼8 nm (FWHM) spectral width. These pulses seed a Tm:fiber based Raman amplifier, which increases the energy up to 9 nJ. The spectrum is broadened up to 40 nm (FWHM) and the center wavelength can be shifted from ∼1.97 - 2.15 μm. The Raman solitons are inherently time-bandwidth limited with pulse durations <150 fs.</EA>
<CC>001B00A30C; 001B40B62; 001B40B65T; 001D17</CC>
<FD>Soliton optique; Amplificateur optique; Résonateur anneau; Optique non linéaire; Application laser; Domaine temps fs; Durée impulsion; Application militaire; 0130C; 4262; 4265T; 8920D; 4260D; Fibre dopée thulium; Amplificateur Raman</FD>
<ED>Optical solitons; Optical amplifier; Ring resonator; Nonlinear optics; Laser beam applications; fs range; Pulse width; Military application; Thulium-doped fibers; Raman amplifier</ED>
<SD>Amplificador óptico; Resonador anillo; Duración impulso; Aplicación militar</SD>
<LO>INIST-21760.354000174755190120</LO>
<ID>12-0011745</ID>
</server>
</inist>
</record>
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