ThuliumV1, Pascal, Corpus, bibRecord, 000096

Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier

Identifieur interne : 000096 ( Pascal/Corpus ); précédent : 000095; suivant : 000097

Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier

Auteurs : A. Zarifi ; S. D. Emami ; F. Z. Zahedi ; H. Fatehi ; S. E. Mirnia ; H. Ahmad ; S. W. Harun

Source :

Optical materials : (Amsterdam) [ 0925-3467 ] ; 2012.

RBID : Pascal:13-0121464

Descripteurs français

Pascal (Inist)
- Transfert énergie excitation, Amplificateur optique, Amplificateur fibre optique, Etude théorique, Méthode analytique, Effet concentration, Rayonnement IR, Puissance sortie, Matériau dopé, Codopage, Addition bismuth, Verre germanate, Matériau optique, Addition thulium, Germanate de bismuth, 4270C, 4260D, Equation bilan transfert énergie.

English descriptors

KwdEn :
- Analytical method, Bismuth additions, Bismuth germanates, Codoping, Doped materials, Excitation energy transfer, Germanate glasses, Infrared radiation, Optical amplifier, Optical fiber amplifiers, Optical materials, Output power, Quantity ratio, Rate equation, Theoretical study, Thulium additions.

Abstract

Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0925-3467`
A03		`1`		`@0 Opt. mater. : (Amst.)`
A05				`@2 35`
A06				`@2 2`
A08	`01`	`1`	`ENG`	`@1 Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier`
A11	`01`	`1`		`@1 ZARIFI (A.)`
A11	`02`	`1`		`@1 EMAMI (S. D.)`
A11	`03`	`1`		`@1 ZAHEDI (F. Z.)`
A11	`04`	`1`		`@1 FATEHI (H.)`
A11	`05`	`1`		`@1 MIRNIA (S. E.)`
A11	`06`	`1`		`@1 AHMAD (H.)`
A11	`07`	`1`		`@1 HARUN (S. W.)`
A14	`01`			`@1 Department of Electrical Engineering, Faculty of Engineering, University of Malaya @2 50603 Kuala Lumpur @3 MYS @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 7 aut.`
A14	`02`			`@1 Photonics Research Center, Department of Physics, University of Malaya @2 50603 Kuala Lumpur @3 MYS @Z 6 aut.`
A20				`@1 231-239`
A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 22598 @5 354000173213410240`
A44				`@0 0000 @1 © 2013 INIST-CNRS. All rights reserved.`
A45				`@0 17 ref.`
A47	`01`	`1`		`@0 13-0121464`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Optical materials : (Amsterdam)`
A66	`01`			`@0 GBR`
C01	`01`		`ENG`	@0 Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.
C02	`01`	`3`		`@0 001B40B60D`
C02	`02`	`3`		`@0 001B40B70C`
C03	`01`	`X`	`FRE`	`@0 Transfert énergie excitation @5 03`
C03	`01`	`X`	`ENG`	`@0 Excitation energy transfer @5 03`
C03	`01`	`X`	`SPA`	`@0 Transferencia energía excitación @5 03`
C03	`02`	`X`	`FRE`	`@0 Amplificateur optique @5 09`
C03	`02`	`X`	`ENG`	`@0 Optical amplifier @5 09`
C03	`02`	`X`	`SPA`	`@0 Amplificador óptico @5 09`
C03	`03`	`3`	`FRE`	`@0 Amplificateur fibre optique @5 11`
C03	`03`	`3`	`ENG`	`@0 Optical fiber amplifiers @5 11`
C03	`04`	`3`	`FRE`	`@0 Etude théorique @5 21`
C03	`04`	`3`	`ENG`	`@0 Theoretical study @5 21`
C03	`05`	`X`	`FRE`	`@0 Méthode analytique @5 23`
C03	`05`	`X`	`ENG`	`@0 Analytical method @5 23`
C03	`05`	`X`	`SPA`	`@0 Método analítico @5 23`
C03	`06`	`3`	`FRE`	`@0 Effet concentration @5 30`
C03	`06`	`3`	`ENG`	`@0 Quantity ratio @5 30`
C03	`07`	`3`	`FRE`	`@0 Rayonnement IR @5 37`
C03	`07`	`3`	`ENG`	`@0 Infrared radiation @5 37`
C03	`08`	`X`	`FRE`	`@0 Puissance sortie @5 41`
C03	`08`	`X`	`ENG`	`@0 Output power @5 41`
C03	`08`	`X`	`SPA`	`@0 Potencia salida @5 41`
C03	`09`	`3`	`FRE`	`@0 Matériau dopé @5 50`
C03	`09`	`3`	`ENG`	`@0 Doped materials @5 50`
C03	`10`	`X`	`FRE`	`@0 Codopage @5 57`
C03	`10`	`X`	`ENG`	`@0 Codoping @5 57`
C03	`10`	`X`	`SPA`	`@0 Codrogado @5 57`
C03	`11`	`3`	`FRE`	`@0 Addition bismuth @5 58`
C03	`11`	`3`	`ENG`	`@0 Bismuth additions @5 58`
C03	`12`	`3`	`FRE`	`@0 Verre germanate @5 59`
C03	`12`	`3`	`ENG`	`@0 Germanate glasses @5 59`
C03	`13`	`3`	`FRE`	`@0 Matériau optique @5 60`
C03	`13`	`3`	`ENG`	`@0 Optical materials @5 60`
C03	`14`	`3`	`FRE`	`@0 Addition thulium @5 61`
C03	`14`	`3`	`ENG`	`@0 Thulium additions @5 61`
C03	`15`	`3`	`FRE`	`@0 Germanate de bismuth @2 NK @5 62`
C03	`15`	`3`	`ENG`	`@0 Bismuth germanates @2 NK @5 62`
C03	`16`	`3`	`FRE`	`@0 4270C @4 INC @5 83`
C03	`17`	`3`	`FRE`	`@0 4260D @4 INC @5 91`
C03	`18`	`3`	`FRE`	`@0 Equation bilan transfert énergie @4 CD @5 96`
C03	`18`	`3`	`ENG`	`@0 Rate equation @4 CD @5 96`
N21				`@1 098`

Format Inist (serveur)

NO :	PASCAL 13-0121464 INIST
ET :	Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier
AU :	ZARIFI (A.); EMAMI (S. D.); ZAHEDI (F. Z.); FATEHI (H.); MIRNIA (S. E.); AHMAD (H.); HARUN (S. W.)
AF :	Department of Electrical Engineering, Faculty of Engineering, University of Malaya/50603 Kuala Lumpur/Malaisie (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 7 aut.); Photonics Research Center, Department of Physics, University of Malaya/50603 Kuala Lumpur/Malaisie (6 aut.)
DT :	Publication en série; Niveau analytique
SO :	Optical materials : (Amsterdam); ISSN 0925-3467; Royaume-Uni; Da. 2012; Vol. 35; No. 2; Pp. 231-239; Bibl. 17 ref.
LA :	Anglais
EA :	Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.
CC :	001B40B60D; 001B40B70C
FD :	Transfert énergie excitation; Amplificateur optique; Amplificateur fibre optique; Etude théorique; Méthode analytique; Effet concentration; Rayonnement IR; Puissance sortie; Matériau dopé; Codopage; Addition bismuth; Verre germanate; Matériau optique; Addition thulium; Germanate de bismuth; 4270C; 4260D; Equation bilan transfert énergie
ED :	Excitation energy transfer; Optical amplifier; Optical fiber amplifiers; Theoretical study; Analytical method; Quantity ratio; Infrared radiation; Output power; Doped materials; Codoping; Bismuth additions; Germanate glasses; Optical materials; Thulium additions; Bismuth germanates; Rate equation
SD :	Transferencia energía excitación; Amplificador óptico; Método analítico; Potencia salida; Codrogado
LO :	INIST-22598.354000173213410240
ID :	13-0121464

Links to Exploration step

Pascal:13-0121464

Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier</title>
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<term>Bismuth additions</term>
<term>Bismuth germanates</term>
<term>Codoping</term>
<term>Doped materials</term>
<term>Excitation energy transfer</term>
<term>Germanate glasses</term>
<term>Infrared radiation</term>
<term>Optical amplifier</term>
<term>Optical fiber amplifiers</term>
<term>Optical materials</term>
<term>Output power</term>
<term>Quantity ratio</term>
<term>Rate equation</term>
<term>Theoretical study</term>
<term>Thulium additions</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Transfert énergie excitation</term>
<term>Amplificateur optique</term>
<term>Amplificateur fibre optique</term>
<term>Etude théorique</term>
<term>Méthode analytique</term>
<term>Effet concentration</term>
<term>Rayonnement IR</term>
<term>Puissance sortie</term>
<term>Matériau dopé</term>
<term>Codopage</term>
<term>Addition bismuth</term>
<term>Verre germanate</term>
<term>Matériau optique</term>
<term>Addition thulium</term>
<term>Germanate de bismuth</term>
<term>4270C</term>
<term>4260D</term>
<term>Equation bilan transfert énergie</term>
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<front><div type="abstract" xml:lang="en">Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.</div>
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<fA14 i1="01"><s1>Department of Electrical Engineering, Faculty of Engineering, University of Malaya</s1>
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<fA14 i1="02"><s1>Photonics Research Center, Department of Physics, University of Malaya</s1>
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<fA64 i1="01" i2="1"><s0>Optical materials : (Amsterdam)</s0>
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<fA66 i1="01"><s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B60D</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B40B70C</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Transfert énergie excitation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Excitation energy transfer</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Transferencia energía excitación</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Amplificateur optique</s0>
<s5>09</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Optical amplifier</s0>
<s5>09</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Amplificador óptico</s0>
<s5>09</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Amplificateur fibre optique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Optical fiber amplifiers</s0>
<s5>11</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Etude théorique</s0>
<s5>21</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Theoretical study</s0>
<s5>21</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Méthode analytique</s0>
<s5>23</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Analytical method</s0>
<s5>23</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Método analítico</s0>
<s5>23</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Effet concentration</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Quantity ratio</s0>
<s5>30</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Rayonnement IR</s0>
<s5>37</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Infrared radiation</s0>
<s5>37</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Puissance sortie</s0>
<s5>41</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Output power</s0>
<s5>41</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Potencia salida</s0>
<s5>41</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>50</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>50</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Codopage</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Codoping</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Codrogado</s0>
<s5>57</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Addition bismuth</s0>
<s5>58</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Bismuth additions</s0>
<s5>58</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Verre germanate</s0>
<s5>59</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Germanate glasses</s0>
<s5>59</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Matériau optique</s0>
<s5>60</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Optical materials</s0>
<s5>60</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Addition thulium</s0>
<s5>61</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Thulium additions</s0>
<s5>61</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Germanate de bismuth</s0>
<s2>NK</s2>
<s5>62</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Bismuth germanates</s0>
<s2>NK</s2>
<s5>62</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>4270C</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>4260D</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Equation bilan transfert énergie</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Rate equation</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>098</s1>
</fN21>
</pA>
</standard>
<server><NO>PASCAL 13-0121464 INIST</NO>
<ET>Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier</ET>
<AU>ZARIFI (A.); EMAMI (S. D.); ZAHEDI (F. Z.); FATEHI (H.); MIRNIA (S. E.); AHMAD (H.); HARUN (S. W.)</AU>
<AF>Department of Electrical Engineering, Faculty of Engineering, University of Malaya/50603 Kuala Lumpur/Malaisie (1 aut., 2 aut., 3 aut., 4 aut., 5 aut., 7 aut.); Photonics Research Center, Department of Physics, University of Malaya/50603 Kuala Lumpur/Malaisie (6 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Optical materials : (Amsterdam); ISSN 0925-3467; Royaume-Uni; Da. 2012; Vol. 35; No. 2; Pp. 231-239; Bibl. 17 ref.</SO>
<LA>Anglais</LA>
<EA>Energy transfer processes in Thulium-Bismuth co-doped germanate fiber amplifier at 1800 nm region have been studied quantitatively in this work. Energy transfer models are utilized in order to investigate the effect of dopants concentration on energy transfer parameters. A series of non-linear rate equations were derived using the energy transfer parameters and solved by means of a semi-analytical method. A general model of optical fiber amplifier in conjunction with rate equations is employed to simulate Thulium and Bismuth ions population distribution along the fiber. Thulium and Bismuth concentrations are noted as critical factors that control the output power and saturation length. The optimum values of Thulium and Bismuth concentration which result in maximum gain at 1800 nm are 0.5 wt.% and 2 wt.% respectively.</EA>
<CC>001B40B60D; 001B40B70C</CC>
<FD>Transfert énergie excitation; Amplificateur optique; Amplificateur fibre optique; Etude théorique; Méthode analytique; Effet concentration; Rayonnement IR; Puissance sortie; Matériau dopé; Codopage; Addition bismuth; Verre germanate; Matériau optique; Addition thulium; Germanate de bismuth; 4270C; 4260D; Equation bilan transfert énergie</FD>
<ED>Excitation energy transfer; Optical amplifier; Optical fiber amplifiers; Theoretical study; Analytical method; Quantity ratio; Infrared radiation; Output power; Doped materials; Codoping; Bismuth additions; Germanate glasses; Optical materials; Thulium additions; Bismuth germanates; Rate equation</ED>
<SD>Transferencia energía excitación; Amplificador óptico; Método analítico; Potencia salida; Codrogado</SD>
<LO>INIST-22598.354000173213410240</LO>
<ID>13-0121464</ID>
</server>
</inist>
</record>

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Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier

Quantitative analysis of energy transfer processes in Thulium-Bismuth germanate co-doped fiber amplifier

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