CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000203

Modeling and analysis of birefringence in magneto-optical thin film made by SiO2/ZrO2 doped with ferrite of cobalt

Identifieur interne : 000203 ( PascalFrancis/Curation ); précédent : 000202; suivant : 000204

Modeling and analysis of birefringence in magneto-optical thin film made by SiO2/ZrO2 doped with ferrite of cobalt

Auteurs : A. Hocini [Algérie] ; T. Boumaza [Algérie] ; M. Bouchemat [Algérie] ; F. Choueikani [France] ; F. Royer [France] ; J. J. Rousseau [France]

Source :

Applied physics. B, Lasers and optics : (Print) [ 0946-2171 ] ; 2010.

RBID : Pascal:10-0271494

Descripteurs français

Pascal (Inist)
- Biréfringence, Adaptation mode, Guide onde optique, Constante propagation, Couche mince, Composé binaire, Silicium Oxyde, Zircone, Ferrite, Cobalt, ZrO2, O Zr, SiO2, O Si, 4225L, 4279G.
Wicri :
- topic : Cobalt.

English descriptors

KwdEn :
- Binary compounds, Birefringence, Cobalt, Ferrite, Mode matching, Optical waveguides, Propagation constant, Silicon Oxides, Thin films, Zirconia.

Abstract

The zero-birefringence condition is an important requirement for magneto-optical waveguide devices. It has been analyzed by means of Film Mode Matching method (FMM). The modelling is based on geometrical adjustments of the rib waveguide and especially the etch depth, which is a critical parameter in the design of rib waveguide. We determine the waveguide dimensions that would allow the same propagation constants for both polarizations TE and TM, and we have found that there are more choices for waveguide dimensions to produce birefringence-free waveguides and single-mode rib waveguide simultaneously.

A01	`01`	`1`		`@0 0946-2171`
A03		`1`		`@0 Appl. phys., B Lasers opt. : (Print)`
A05				`@2 99`
A06				`@2 3`
A08	`01`	`1`	`ENG`	`@1 Modeling and analysis of birefringence in magneto-optical thin film made by SiO₂/ZrO₂ doped with ferrite of cobalt`
A11	`01`	`1`		`@1 HOCINI (A.)`
A11	`02`	`1`		`@1 BOUMAZA (T.)`
A11	`03`	`1`		`@1 BOUCHEMAT (M.)`
A11	`04`	`1`		`@1 CHOUEIKANI (F.)`
A11	`05`	`1`		`@1 ROYER (F.)`
A11	`06`	`1`		`@1 ROUSSEAU (J. J.)`
A14	`01`			`@1 Laboratoire Micro Systèmes et Instrumentation, Département d'Électronique, Université de Constantine, route d'Aïn el Bey @2 Constantine @3 DZA @Z 1 aut. @Z 2 aut. @Z 3 aut.`
A14	`02`			`@1 Laboratoire Dispositifs et Instrumentation en Optoélectronique et Micro-ondes-EA 3523, Université Jean Monnet, 21 rue Paul Michelon @2 42023 St Etienne @3 FRA @Z 4 aut. @Z 5 aut. @Z 6 aut.`
A20				`@1 553-558`
A21				`@1 2010`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 16194B @5 354000192979030260`
A44				`@0 0000 @1 © 2010 INIST-CNRS. All rights reserved.`
A45				`@0 10 ref.`
A47	`01`	`1`		`@0 10-0271494`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Applied physics. B, Lasers and optics : (Print)`
A66	`01`			`@0 DEU`
C01	`01`		`ENG`	@0 The zero-birefringence condition is an important requirement for magneto-optical waveguide devices. It has been analyzed by means of Film Mode Matching method (FMM). The modelling is based on geometrical adjustments of the rib waveguide and especially the etch depth, which is a critical parameter in the design of rib waveguide. We determine the waveguide dimensions that would allow the same propagation constants for both polarizations TE and TM, and we have found that there are more choices for waveguide dimensions to produce birefringence-free waveguides and single-mode rib waveguide simultaneously.
C02	`01`	`3`		`@0 001B40B25L`
C02	`02`	`3`		`@0 001B40B79G`
C03	`01`	`3`	`FRE`	`@0 Biréfringence @5 03`
C03	`01`	`3`	`ENG`	`@0 Birefringence @5 03`
C03	`02`	`3`	`FRE`	`@0 Adaptation mode @5 04`
C03	`02`	`3`	`ENG`	`@0 Mode matching @5 04`
C03	`03`	`3`	`FRE`	`@0 Guide onde optique @5 11`
C03	`03`	`3`	`ENG`	`@0 Optical waveguides @5 11`
C03	`04`	`X`	`FRE`	`@0 Constante propagation @5 41`
C03	`04`	`X`	`ENG`	`@0 Propagation constant @5 41`
C03	`04`	`X`	`SPA`	`@0 Constante propagación @5 41`
C03	`05`	`3`	`FRE`	`@0 Couche mince @5 47`
C03	`05`	`3`	`ENG`	`@0 Thin films @5 47`
C03	`06`	`3`	`FRE`	`@0 Composé binaire @5 50`
C03	`06`	`3`	`ENG`	`@0 Binary compounds @5 50`
C03	`07`	`3`	`FRE`	`@0 Silicium Oxyde @2 NC @5 51`
C03	`07`	`3`	`ENG`	`@0 Silicon Oxides @2 NC @5 51`
C03	`08`	`X`	`FRE`	`@0 Zircone @5 52`
C03	`08`	`X`	`ENG`	`@0 Zirconia @5 52`
C03	`08`	`X`	`SPA`	`@0 Zircona @5 52`
C03	`09`	`3`	`FRE`	`@0 Ferrite @5 61`
C03	`09`	`3`	`ENG`	`@0 Ferrite @5 61`
C03	`10`	`3`	`FRE`	`@0 Cobalt @2 NC @5 62`
C03	`10`	`3`	`ENG`	`@0 Cobalt @2 NC @5 62`
C03	`11`	`3`	`FRE`	`@0 ZrO2 @4 INC @5 71`
C03	`12`	`3`	`FRE`	`@0 O Zr @4 INC @5 75`
C03	`13`	`3`	`FRE`	`@0 SiO2 @4 INC @5 83`
C03	`14`	`3`	`FRE`	`@0 O Si @4 INC @5 84`
C03	`15`	`3`	`FRE`	`@0 4225L @4 INC @5 91`
C03	`16`	`3`	`FRE`	`@0 4279G @4 INC @5 92`
N21				`@1 172`
N44	`01`			`@1 OTO`
N82				`@1 OTO`

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Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Modeling and analysis of birefringence in magneto-optical thin film made by SiO<sub>2</sub>
/ZrO<sub>2</sub>
 doped with ferrite of cobalt</title>
<author><name sortKey="Hocini, A" sort="Hocini, A" uniqKey="Hocini A" first="A." last="Hocini">A. Hocini</name>
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<author><name sortKey="Boumaza, T" sort="Boumaza, T" uniqKey="Boumaza T" first="T." last="Boumaza">T. Boumaza</name>
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<s2>Constantine</s2>
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<author><name sortKey="Choueikani, F" sort="Choueikani, F" uniqKey="Choueikani F" first="F." last="Choueikani">F. Choueikani</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Dispositifs et Instrumentation en Optoélectronique et Micro-ondes-EA 3523, Université Jean Monnet, 21 rue Paul Michelon</s1>
<s2>42023 St Etienne</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
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<author><name sortKey="Royer, F" sort="Royer, F" uniqKey="Royer F" first="F." last="Royer">F. Royer</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire Dispositifs et Instrumentation en Optoélectronique et Micro-ondes-EA 3523, Université Jean Monnet, 21 rue Paul Michelon</s1>
<s2>42023 St Etienne</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
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<author><name sortKey="Rousseau, J J" sort="Rousseau, J J" uniqKey="Rousseau J" first="J. J." last="Rousseau">J. J. Rousseau</name>
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<s2>42023 St Etienne</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
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<series><title level="j" type="main">Applied physics. B, Lasers and optics : (Print)</title>
<title level="j" type="abbreviated">Appl. phys., B Lasers opt. : (Print)</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Binary compounds</term>
<term>Birefringence</term>
<term>Cobalt</term>
<term>Ferrite</term>
<term>Mode matching</term>
<term>Optical waveguides</term>
<term>Propagation constant</term>
<term>Silicon Oxides</term>
<term>Thin films</term>
<term>Zirconia</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Biréfringence</term>
<term>Adaptation mode</term>
<term>Guide onde optique</term>
<term>Constante propagation</term>
<term>Couche mince</term>
<term>Composé binaire</term>
<term>Silicium Oxyde</term>
<term>Zircone</term>
<term>Ferrite</term>
<term>Cobalt</term>
<term>ZrO2</term>
<term>O Zr</term>
<term>SiO2</term>
<term>O Si</term>
<term>4225L</term>
<term>4279G</term>
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<front><div type="abstract" xml:lang="en">The zero-birefringence condition is an important requirement for magneto-optical waveguide devices. It has been analyzed by means of Film Mode Matching method (FMM). The modelling is based on geometrical adjustments of the rib waveguide and especially the etch depth, which is a critical parameter in the design of rib waveguide. We determine the waveguide dimensions that would allow the same propagation constants for both polarizations TE and TM, and we have found that there are more choices for waveguide dimensions to produce birefringence-free waveguides and single-mode rib waveguide simultaneously.</div>
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<fA08 i1="01" i2="1" l="ENG"><s1>Modeling and analysis of birefringence in magneto-optical thin film made by SiO<sub>2</sub>
/ZrO<sub>2</sub>
 doped with ferrite of cobalt</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>HOCINI (A.)</s1>
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<fA14 i1="01"><s1>Laboratoire Micro Systèmes et Instrumentation, Département d'Électronique, Université de Constantine, route d'Aïn el Bey</s1>
<s2>Constantine</s2>
<s3>DZA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Laboratoire Dispositifs et Instrumentation en Optoélectronique et Micro-ondes-EA 3523, Université Jean Monnet, 21 rue Paul Michelon</s1>
<s2>42023 St Etienne</s2>
<s3>FRA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
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</fA66>
<fC01 i1="01" l="ENG"><s0>The zero-birefringence condition is an important requirement for magneto-optical waveguide devices. It has been analyzed by means of Film Mode Matching method (FMM). The modelling is based on geometrical adjustments of the rib waveguide and especially the etch depth, which is a critical parameter in the design of rib waveguide. We determine the waveguide dimensions that would allow the same propagation constants for both polarizations TE and TM, and we have found that there are more choices for waveguide dimensions to produce birefringence-free waveguides and single-mode rib waveguide simultaneously.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B25L</s0>
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<fC02 i1="02" i2="3"><s0>001B40B79G</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Biréfringence</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Birefringence</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Adaptation mode</s0>
<s5>04</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Mode matching</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Guide onde optique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Optical waveguides</s0>
<s5>11</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Constante propagation</s0>
<s5>41</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Propagation constant</s0>
<s5>41</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Constante propagación</s0>
<s5>41</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Couche mince</s0>
<s5>47</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Thin films</s0>
<s5>47</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Composé binaire</s0>
<s5>50</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Binary compounds</s0>
<s5>50</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Silicium Oxyde</s0>
<s2>NC</s2>
<s5>51</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Silicon Oxides</s0>
<s2>NC</s2>
<s5>51</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Zircone</s0>
<s5>52</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Zirconia</s0>
<s5>52</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Zircona</s0>
<s5>52</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Ferrite</s0>
<s5>61</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Ferrite</s0>
<s5>61</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>62</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>62</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>ZrO2</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>O Zr</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>SiO2</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>O Si</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>4225L</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>4279G</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fN21><s1>172</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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	Serveur d'exploration sur le cobalt au Maghreb
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Serveur d'exploration sur le cobalt au Maghreb

Modeling and analysis of birefringence in magneto-optical thin film made by SiO2/ZrO2 doped with ferrite of cobalt

Modeling and analysis of birefringence in magneto-optical thin film made by SiO2/ZrO2 doped with ferrite of cobalt

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