ThuliumV1, Pascal, Curation, bibRecord, 000188

Atmospheric gas detection using broadband mid-IR thulium fiber-based sources

Identifieur interne : 000188 ( Pascal/Curation ); précédent : 000187; suivant : 000189

Atmospheric gas detection using broadband mid-IR thulium fiber-based sources

Auteurs : Pankaj Kadwani [États-Unis] ; Robert A. Sims [États-Unis] ; Jeffrey Chia [États-Unis] ; Falah Altal [Émirats arabes unis] ; Lawrence Shah [États-Unis] ; Martin C. Richardson [États-Unis]

Source :

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

RBID : Pascal:12-0011743

Descripteurs français

Pascal (Inist)
- Amplificateur optique, Elément optique, Application laser, Rayonnement IR moyen, Densité spectrale, Thulium, Application militaire, CO2, 0130C, 4262, 8920D, 4260D, Amplificateur Raman.

English descriptors

KwdEn :
- Laser beam applications, Mid infrared radiation, Military application, Optical amplifier, Optical elements, Raman amplifier, Spectral density, Thulium.

Abstract

We present a Tm:fiber based broadband ASE source which was used for atmospheric CO₂ detection. The average spectral power of this source was limited to ∼6.1 μW/nm which was the main limitation in detection of trace concentrations of gases. This shortcoming was overcome by using an ultrashort pulsed Raman amplifier system with maximum of ∼127 μW/nm of spectral power density which was able to provide sensitivity better than 300 ppm for CO₂. In addition, improving the average power of the ASE provided an essential tool in lab to characterize optical elements with sharp spectral features around 2 μm.

A01	`01`	`1`		`@0 0277-786X`
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A03		`1`		`@0 Proc. SPIE Int. Soc. Opt. Eng.`
A05				`@2 8039`
A08	`01`	`1`	`ENG`	`@1 Atmospheric gas detection using broadband mid-IR thulium fiber-based sources`
A09	`01`	`1`	`ENG`	`@1 Laser technology for defense and security VII : 25-27 April 2011, Orlando, Florida, United States`
A11	`01`	`1`		`@1 KADWANI (Pankaj)`
A11	`02`	`1`		`@1 SIMS (Robert A.)`
A11	`03`	`1`		`@1 CHIA (Jeffrey)`
A11	`04`	`1`		`@1 ALTAL (Falah)`
A11	`05`	`1`		`@1 SHAH (Lawrence)`
A11	`06`	`1`		`@1 RICHARDSON (Martin C.)`
A12	`01`	`1`		`@1 DUBINSKII (Mark A.) @9 ed.`
A12	`02`	`1`		`@1 POST (Stephen G.) @9 ed.`
A14	`01`			`@1 CREOL College of Optics and Photonics, University of Central Florida, 4000 Central Florida Blvd @2 Orlando, FL, 32816 @3 USA @Z 1 aut. @Z 2 aut. @Z 5 aut. @Z 6 aut.`
A14	`02`			`@1 College of Optical Sciences, The university of Arizona @2 Tucson, AZ, 85721 @3 USA @Z 3 aut.`
A14	`03`			`@1 Masdar Institute of Science and Technology, PO Box 54224 @2 Abu Dhabi @3 ARE @Z 4 aut.`
A18	`01`	`1`		`@1 SPIE @3 USA @9 org-cong.`
A20				`@2 80390L.1-80390L.5`
A21				`@1 2011`
A23	`01`			`@0 ENG`
A25	`01`			`@1 SPIE @2 Bellingham WA`
A26	`01`			`@0 978-0-8194-8613-4`
A43	`01`			`@1 INIST @2 21760 @5 354000174755190130`
A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 5 ref.`
A47	`01`	`1`		`@0 12-0011743`
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 We present a Tm:fiber based broadband ASE source which was used for atmospheric CO₂ detection. The average spectral power of this source was limited to ∼6.1 μW/nm which was the main limitation in detection of trace concentrations of gases. This shortcoming was overcome by using an ultrashort pulsed Raman amplifier system with maximum of ∼127 μW/nm of spectral power density which was able to provide sensitivity better than 300 ppm for CO₂. In addition, improving the average power of the ASE provided an essential tool in lab to characterize optical elements with sharp spectral features around 2 μm.
C02	`01`	`3`		`@0 001B00A30C`
C02	`02`	`3`		`@0 001B40B62`
C02	`03`	`X`		`@0 001D17`
C02	`04`	`3`		`@0 001B40B60D`
C03	`01`	`X`	`FRE`	`@0 Amplificateur optique @5 09`
C03	`01`	`X`	`ENG`	`@0 Optical amplifier @5 09`
C03	`01`	`X`	`SPA`	`@0 Amplificador óptico @5 09`
C03	`02`	`3`	`FRE`	`@0 Elément optique @5 11`
C03	`02`	`3`	`ENG`	`@0 Optical elements @5 11`
C03	`03`	`3`	`FRE`	`@0 Application laser @5 19`
C03	`03`	`3`	`ENG`	`@0 Laser beam applications @5 19`
C03	`04`	`X`	`FRE`	`@0 Rayonnement IR moyen @5 37`
C03	`04`	`X`	`ENG`	`@0 Mid infrared radiation @5 37`
C03	`04`	`X`	`SPA`	`@0 Radiación infrarroja media @5 37`
C03	`05`	`3`	`FRE`	`@0 Densité spectrale @5 41`
C03	`05`	`3`	`ENG`	`@0 Spectral density @5 41`
C03	`06`	`3`	`FRE`	`@0 Thulium @2 NC @5 61`
C03	`06`	`3`	`ENG`	`@0 Thulium @2 NC @5 61`
C03	`07`	`X`	`FRE`	`@0 Application militaire @5 62`
C03	`07`	`X`	`ENG`	`@0 Military application @5 62`
C03	`07`	`X`	`SPA`	`@0 Aplicación militar @5 62`
C03	`08`	`3`	`FRE`	`@0 CO2 @4 INC @5 83`
C03	`09`	`3`	`FRE`	`@0 0130C @4 INC @5 84`
C03	`10`	`3`	`FRE`	`@0 4262 @4 INC @5 85`
C03	`11`	`3`	`FRE`	`@0 8920D @4 INC @5 91`
C03	`12`	`3`	`FRE`	`@0 4260D @4 INC @5 92`
C03	`13`	`3`	`FRE`	`@0 Amplificateur Raman @4 CD @5 96`
C03	`13`	`3`	`ENG`	`@0 Raman amplifier @4 CD @5 96`
N21				`@1 002`
N44	`01`			`@1 OTO`
N82				`@1 OTO`

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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Le document en format XML

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<front><div type="abstract" xml:lang="en">We present a Tm:fiber based broadband ASE source which was used for atmospheric CO<sub>2</sub>
 detection. The average spectral power of this source was limited to ∼6.1 μW/nm which was the main limitation in detection of trace concentrations of gases. This shortcoming was overcome by using an ultrashort pulsed Raman amplifier system with maximum of ∼127 μW/nm of spectral power density which was able to provide sensitivity better than 300 ppm for CO<sub>2</sub>
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 detection. The average spectral power of this source was limited to ∼6.1 μW/nm which was the main limitation in detection of trace concentrations of gases. This shortcoming was overcome by using an ultrashort pulsed Raman amplifier system with maximum of ∼127 μW/nm of spectral power density which was able to provide sensitivity better than 300 ppm for CO<sub>2</sub>
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<s5>62</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>CO2</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>4262</s0>
<s4>INC</s4>
<s5>85</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>8920D</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>4260D</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Amplificateur Raman</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Raman amplifier</s0>
<s4>CD</s4>
<s5>96</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>
</inist>
</record>

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Atmospheric gas detection using broadband mid-IR thulium fiber-based sources

Atmospheric gas detection using broadband mid-IR thulium fiber-based sources

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