ThuliumV1, Pascal, Corpus, bibRecord, 000217

Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber

Identifieur interne : 000217 ( Pascal/Corpus ); précédent : 000216; suivant : 000218

Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber

Auteurs : R. Andrew Sims ; Pankaj Kadwani ; Lawrence Shah ; Martin Richardson

Source :

Proceedings of SPIE, the International Society for Optical Engineering [ 0277-786X ] ; 2011.

RBID : Pascal:11-0365459

Descripteurs français

Pascal (Inist)
- Impulsion ultracourte, Traitement matériau, Blocage mode laser, Soliton optique, Compensation dispersion optique, Laser pulsé, Laser fibre, Optique non linéaire, Domaine temps fs, Sécurité oculaire, Fibre optique, Nanotube monofeuillet, Nanotube carbone, Matériau dopé, Silice, Addition thulium, Absorbant saturable, Largeur bande spectrale, 0130C, 4265R, 4260F, 4265T, 4255W.

English descriptors

KwdEn :
- Carbon nanotubes, Doped materials, Eye safety, Fiber lasers, Laser mode locking, Material processing, Nonlinear optics, Optical dispersion compensation, Optical fibers, Optical solitons, Pulsed lasers, Saturable absorbers, Silica, Singlewalled nanotube, Spectral bandwidth, Thulium additions, Ultrashort pulse, fs range.

Abstract

Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0277-786X`
A02	`01`			`@0 PSISDG`
A03		`1`		`@0 Proc. SPIE Int. Soc. Opt. Eng.`
A05				`@2 7914`
A08	`01`	`1`	`ENG`	`@1 Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber`
A09	`01`	`1`	`ENG`	`@1 Fiber lasers VIII : technology, systems, and applications`
A11	`01`	`1`		`@1 SIMS (R. Andrew)`
A11	`02`	`1`		`@1 KADWANI (Pankaj)`
A11	`03`	`1`		`@1 SHAH (Lawrence)`
A11	`04`	`1`		`@1 RICHARDSON (Martin)`
A12	`01`	`1`		`@1 DAWSON (Jay W.) @9 ed.`
A12	`02`	`1`		`@1 HONEA (Eric C.) @9 ed.`
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.`
A18	`01`	`1`		`@1 SPIE @3 USA @9 org-cong.`
A20				`@2 79141L.1-79141L.6`
A21				`@1 2011`
A23	`01`			`@0 ENG`
A25	`01`			`@1 SPIE @2 Bellingham, Wash.`
A26	`01`			`@0 978-0-8194-8451-2`
A43	`01`			`@1 INIST @2 21760 @5 354000174739020440`
A44				`@0 0000 @1 © 2011 INIST-CNRS. All rights reserved.`
A45				`@0 8 ref.`
A47	`01`	`1`		`@0 11-0365459`
A60				`@1 P @2 C`
A61				`@0 A`
A64	`01`	`1`		`@0 Proceedings of SPIE, the International Society for Optical Engineering`
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C01	`01`		`ENG`	@0 Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.
C02	`01`	`3`		`@0 001B00A30C`
C02	`02`	`3`		`@0 001B40B65R`
C02	`03`	`3`		`@0 001B40B60F`
C02	`04`	`3`		`@0 001B40B65T`
C03	`01`	`X`	`FRE`	`@0 Impulsion ultracourte @5 03`
C03	`01`	`X`	`ENG`	`@0 Ultrashort pulse @5 03`
C03	`01`	`X`	`SPA`	`@0 Impulsión ultracorto @5 03`
C03	`02`	`X`	`FRE`	`@0 Traitement matériau @5 04`
C03	`02`	`X`	`ENG`	`@0 Material processing @5 04`
C03	`02`	`X`	`SPA`	`@0 Tratamiento material @5 04`
C03	`03`	`3`	`FRE`	`@0 Blocage mode laser @5 05`
C03	`03`	`3`	`ENG`	`@0 Laser mode locking @5 05`
C03	`04`	`3`	`FRE`	`@0 Soliton optique @5 06`
C03	`04`	`3`	`ENG`	`@0 Optical solitons @5 06`
C03	`05`	`3`	`FRE`	`@0 Compensation dispersion optique @5 07`
C03	`05`	`3`	`ENG`	`@0 Optical dispersion compensation @5 07`
C03	`06`	`3`	`FRE`	`@0 Laser pulsé @5 11`
C03	`06`	`3`	`ENG`	`@0 Pulsed lasers @5 11`
C03	`07`	`3`	`FRE`	`@0 Laser fibre @5 12`
C03	`07`	`3`	`ENG`	`@0 Fiber lasers @5 12`
C03	`08`	`3`	`FRE`	`@0 Optique non linéaire @5 17`
C03	`08`	`3`	`ENG`	`@0 Nonlinear optics @5 17`
C03	`09`	`3`	`FRE`	`@0 Domaine temps fs @5 41`
C03	`09`	`3`	`ENG`	`@0 fs range @5 41`
C03	`10`	`X`	`FRE`	`@0 Sécurité oculaire @5 42`
C03	`10`	`X`	`ENG`	`@0 Eye safety @5 42`
C03	`10`	`X`	`SPA`	`@0 Seguridad ocular @5 42`
C03	`11`	`3`	`FRE`	`@0 Fibre optique @5 47`
C03	`11`	`3`	`ENG`	`@0 Optical fibers @5 47`
C03	`12`	`3`	`FRE`	`@0 Nanotube monofeuillet @5 48`
C03	`12`	`3`	`ENG`	`@0 Singlewalled nanotube @5 48`
C03	`13`	`3`	`FRE`	`@0 Nanotube carbone @5 49`
C03	`13`	`3`	`ENG`	`@0 Carbon nanotubes @5 49`
C03	`14`	`3`	`FRE`	`@0 Matériau dopé @5 50`
C03	`14`	`3`	`ENG`	`@0 Doped materials @5 50`
C03	`15`	`3`	`FRE`	`@0 Silice @2 NK @5 57`
C03	`15`	`3`	`ENG`	`@0 Silica @2 NK @5 57`
C03	`16`	`3`	`FRE`	`@0 Addition thulium @5 61`
C03	`16`	`3`	`ENG`	`@0 Thulium additions @5 61`
C03	`17`	`3`	`FRE`	`@0 Absorbant saturable @5 62`
C03	`17`	`3`	`ENG`	`@0 Saturable absorbers @5 62`
C03	`18`	`X`	`FRE`	`@0 Largeur bande spectrale @5 63`
C03	`18`	`X`	`ENG`	`@0 Spectral bandwidth @5 63`
C03	`18`	`X`	`SPA`	`@0 Anchura banda espectral @5 63`
C03	`19`	`3`	`FRE`	`@0 0130C @4 INC @5 83`
C03	`20`	`3`	`FRE`	`@0 4265R @4 INC @5 91`
C03	`21`	`3`	`FRE`	`@0 4260F @4 INC @5 92`
C03	`22`	`3`	`FRE`	`@0 4265T @4 INC @5 93`
C03	`23`	`3`	`FRE`	`@0 4255W @4 INC @5 94`
N21				`@1 249`
N44	`01`			`@1 OTO`
N82				`@1 OTO`

A30	`01`	`1`	`ENG`	`@1 Fiber lasers @2 08 @3 San Francisco CA USA @4 2011`

Format Inist (serveur)

NO :	PASCAL 11-0365459 INIST
ET :	Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber
AU :	SIMS (R. Andrew); KADWANI (Pankaj); SHAH (Lawrence); RICHARDSON (Martin); DAWSON (Jay W.); HONEA (Eric C.)
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. 7914; 79141L.1-79141L.6; Bibl. 8 ref.
LA :	Anglais
EA :	Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.
CC :	001B00A30C; 001B40B65R; 001B40B60F; 001B40B65T
FD :	Impulsion ultracourte; Traitement matériau; Blocage mode laser; Soliton optique; Compensation dispersion optique; Laser pulsé; Laser fibre; Optique non linéaire; Domaine temps fs; Sécurité oculaire; Fibre optique; Nanotube monofeuillet; Nanotube carbone; Matériau dopé; Silice; Addition thulium; Absorbant saturable; Largeur bande spectrale; 0130C; 4265R; 4260F; 4265T; 4255W
ED :	Ultrashort pulse; Material processing; Laser mode locking; Optical solitons; Optical dispersion compensation; Pulsed lasers; Fiber lasers; Nonlinear optics; fs range; Eye safety; Optical fibers; Singlewalled nanotube; Carbon nanotubes; Doped materials; Silica; Thulium additions; Saturable absorbers; Spectral bandwidth
SD :	Impulsión ultracorto; Tratamiento material; Seguridad ocular; Anchura banda espectral
LO :	INIST-21760.354000174739020440
ID :	11-0365459

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Pascal:11-0365459

Le document en format XML

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<term>Laser pulsé</term>
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<front><div type="abstract" xml:lang="en">Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.</div>
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<fC01 i1="01" l="ENG"><s0>Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.</s0>
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<s5>05</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Laser mode locking</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Soliton optique</s0>
<s5>06</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Optical solitons</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Compensation dispersion optique</s0>
<s5>07</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Optical dispersion compensation</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Laser pulsé</s0>
<s5>11</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Pulsed lasers</s0>
<s5>11</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Laser fibre</s0>
<s5>12</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Fiber lasers</s0>
<s5>12</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Optique non linéaire</s0>
<s5>17</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Nonlinear optics</s0>
<s5>17</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Domaine temps fs</s0>
<s5>41</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>fs range</s0>
<s5>41</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Sécurité oculaire</s0>
<s5>42</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Eye safety</s0>
<s5>42</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Seguridad ocular</s0>
<s5>42</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Fibre optique</s0>
<s5>47</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Optical fibers</s0>
<s5>47</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Nanotube monofeuillet</s0>
<s5>48</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Singlewalled nanotube</s0>
<s5>48</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Nanotube carbone</s0>
<s5>49</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Carbon nanotubes</s0>
<s5>49</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>50</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>50</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Silice</s0>
<s2>NK</s2>
<s5>57</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Silica</s0>
<s2>NK</s2>
<s5>57</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>61</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>61</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Absorbant saturable</s0>
<s5>62</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Saturable absorbers</s0>
<s5>62</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE"><s0>Largeur bande spectrale</s0>
<s5>63</s5>
</fC03>
<fC03 i1="18" i2="X" l="ENG"><s0>Spectral bandwidth</s0>
<s5>63</s5>
</fC03>
<fC03 i1="18" i2="X" l="SPA"><s0>Anchura banda espectral</s0>
<s5>63</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>4265R</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>4260F</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>4265T</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>4255W</s0>
<s4>INC</s4>
<s5>94</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>Fiber lasers</s1>
<s2>08</s2>
<s3>San Francisco CA USA</s3>
<s4>2011</s4>
</fA30>
</pR>
</standard>
<server><NO>PASCAL 11-0365459 INIST</NO>
<ET>Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber</ET>
<AU>SIMS (R. Andrew); KADWANI (Pankaj); SHAH (Lawrence); RICHARDSON (Martin); DAWSON (Jay W.); HONEA (Eric C.)</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. 7914; 79141L.1-79141L.6; Bibl. 8 ref.</SO>
<LA>Anglais</LA>
<EA>Amplified ultrashort pulses at 2 μm are of great interest for atmospheric sensing, medical, and materials processing applications. We describe the generation and amplification of femtosecond 2 μm pulses in thulium doped silica fiber. Mode-locked eye-safe laser pulses at ∼2 μm were generated in a Tm:fiber oscillator using a single-walled carbon nanotube saturable absorber. Stable mode-locking was achieved at a repetition rate of 70 MHz with soliton pulses reaching energies of ∼40 pJ with a spectral bandwidth of ∼8 nm. Autocorrelation measurements indicated bandwidth limited pulses of ∼500 fs duration. This oscillator was used to seed a Tm:fiber amplifier in both free space and fiber coupled configurations. Effects of dispersion compensation and pulse amplification are reported.</EA>
<CC>001B00A30C; 001B40B65R; 001B40B60F; 001B40B65T</CC>
<FD>Impulsion ultracourte; Traitement matériau; Blocage mode laser; Soliton optique; Compensation dispersion optique; Laser pulsé; Laser fibre; Optique non linéaire; Domaine temps fs; Sécurité oculaire; Fibre optique; Nanotube monofeuillet; Nanotube carbone; Matériau dopé; Silice; Addition thulium; Absorbant saturable; Largeur bande spectrale; 0130C; 4265R; 4260F; 4265T; 4255W</FD>
<ED>Ultrashort pulse; Material processing; Laser mode locking; Optical solitons; Optical dispersion compensation; Pulsed lasers; Fiber lasers; Nonlinear optics; fs range; Eye safety; Optical fibers; Singlewalled nanotube; Carbon nanotubes; Doped materials; Silica; Thulium additions; Saturable absorbers; Spectral bandwidth</ED>
<SD>Impulsión ultracorto; Tratamiento material; Seguridad ocular; Anchura banda espectral</SD>
<LO>INIST-21760.354000174739020440</LO>
<ID>11-0365459</ID>
</server>
</inist>
</record>

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Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber

Generation and Amplification of 350 fs, 2 μm pulses in Tm:fiber

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