Correlation of GMR with texture and interfacial roughness in optimized rf sputtering deposited Co/Cu multilayers
Identifieur interne :
000368 ( PascalFrancis/Curation );
précédent :
000367;
suivant :
000369
Correlation of GMR with texture and interfacial roughness in optimized rf sputtering deposited Co/Cu multilayers
Auteurs : J. Ben Youssef [
France,
Maroc] ;
K. Bouziane [
France] ;
O. Koshkina [
France] ;
H. Le Gall [
France] ;
M. El Harfaoui [
Maroc] ;
M. El Yamani [
Maroc] ;
J. M. Desvignes [
France] ;
A. Fert [
France]
Source :
-
Journal of magnetism and magnetic materials [ 0304-8853 ] ; 1997.
RBID : Pascal:97-0157111
Descripteurs français
- Pascal (Inist)
- Magnétorésistance géante,
Texture,
Rugosité,
Interface solide solide,
Multicouche,
XRD,
Résonance antiferromagnétique,
Effet dimensionnel,
Epaisseur,
Etude expérimentale,
Oscillation,
Préparation,
Pulvérisation haute fréquence,
Cobalt,
Cuivre,
7570P,
6835C,
Co,
Cu.
- Wicri :
English descriptors
- KwdEn :
- Antiferromagnetic resonance,
Cobalt,
Copper,
Experimental study,
Giant magnetoresistance,
Multilayers,
Oscillations,
Preparation,
Radiofrequency sputtering,
Roughness,
Size effect,
Solid-solid interfaces,
Texture,
Thickness,
XRD.
Abstract
Copyright (c) 1996 Elsevier Science B.V. All rights reserved. The objectives of the present work were two fold: first to obtain the highest giant magnetoresistance (GMR) ratio in Co/Cu multilayers grown from the unusual process of rf diode sputtering and second, to investigate in detail correlation between GMR and texture and the interfacial roughness deduced from X-ray diffraction and AFM, respectively. Different interface structures have been induced from the change of the sputtering parameters (sputtering argon gas pressure PAr) which gave the optimal rf sputtering conditions for high GMR. From different results it is concluded that the most important parameter is interface roughness which induces a strong effect on both the GMR and the resistivity of the superlattice. A change in the tCo2 dependence of the reciprocal resistance near tCo=25 Å is attributed to an increase of the effect of the layer roughness when the tCo is going from mesoscopic (tCo>25 Å) to nanoscopic scale (tCo<25 Å).
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A08 | 01 | 1 | ENG | @1 Correlation of GMR with texture and interfacial roughness in optimized rf sputtering deposited Co/Cu multilayers |
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A11 | 01 | 1 | | @1 BEN YOUSSEF (J.) |
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A11 | 02 | 1 | | @1 BOUZIANE (K.) |
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A11 | 03 | 1 | | @1 KOSHKINA (O.) |
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A11 | 04 | 1 | | @1 LE GALL (H.) |
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A11 | 05 | 1 | | @1 EL HARFAOUI (M.) |
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A11 | 06 | 1 | | @1 EL YAMANI (M.) |
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A11 | 07 | 1 | | @1 DESVIGNES (J. M.) |
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A11 | 08 | 1 | | @1 FERT (A.) |
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A20 | | | | @1 288-291 |
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A21 | | | | @1 1997 |
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A23 | 01 | | | @0 ENG |
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A24 | 01 | | | @0 eng |
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A43 | 01 | | | @1 INIST @2 17230 @5 354000063124420138 |
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A44 | | | | @0 9000 @1 © 1997 Elsevier Science B.V. All rights reserved. |
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A47 | 01 | 1 | | @0 97-0157111 |
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A60 | | | | @1 P @2 C |
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A61 | | | | @0 A |
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A64 | 01 | 1 | | @0 Journal of magnetism and magnetic materials |
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A66 | 01 | | | @0 NLD |
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C01 | 01 | | ENG | @0 Copyright (c) 1996 Elsevier Science B.V. All rights reserved. The objectives of the present work were two fold: first to obtain the highest giant magnetoresistance (GMR) ratio in Co/Cu multilayers grown from the unusual process of rf diode sputtering and second, to investigate in detail correlation between GMR and texture and the interfacial roughness deduced from X-ray diffraction and AFM, respectively. Different interface structures have been induced from the change of the sputtering parameters (sputtering argon gas pressure PAr) which gave the optimal rf sputtering conditions for high GMR. From different results it is concluded that the most important parameter is interface roughness which induces a strong effect on both the GMR and the resistivity of the superlattice. A change in the tCo2 dependence of the reciprocal resistance near tCo=25 Å is attributed to an increase of the effect of the layer roughness when the tCo is going from mesoscopic (tCo>25 Å) to nanoscopic scale (tCo<25 Å). |
---|
C02 | 01 | 3 | | @0 001B70E70P |
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C02 | 02 | 3 | | @0 001B60H35C |
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C02 | 03 | X | | @0 240 |
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C03 | 01 | 3 | FRE | @0 Magnétorésistance géante @5 01 |
---|
C03 | 01 | 3 | ENG | @0 Giant magnetoresistance @5 01 |
---|
C03 | 02 | 3 | FRE | @0 Texture @5 02 |
---|
C03 | 02 | 3 | ENG | @0 Texture @5 02 |
---|
C03 | 03 | 3 | FRE | @0 Rugosité @5 03 |
---|
C03 | 03 | 3 | ENG | @0 Roughness @5 03 |
---|
C03 | 04 | 3 | FRE | @0 Interface solide solide @5 04 |
---|
C03 | 04 | 3 | ENG | @0 Solid-solid interfaces @5 04 |
---|
C03 | 05 | 3 | FRE | @0 Multicouche @5 05 |
---|
C03 | 05 | 3 | ENG | @0 Multilayers @5 05 |
---|
C03 | 06 | 3 | FRE | @0 XRD @5 06 |
---|
C03 | 06 | 3 | ENG | @0 XRD @5 06 |
---|
C03 | 07 | 3 | FRE | @0 Résonance antiferromagnétique @5 07 |
---|
C03 | 07 | 3 | ENG | @0 Antiferromagnetic resonance @5 07 |
---|
C03 | 08 | 3 | FRE | @0 Effet dimensionnel @5 08 |
---|
C03 | 08 | 3 | ENG | @0 Size effect @5 08 |
---|
C03 | 09 | 3 | FRE | @0 Epaisseur @5 09 |
---|
C03 | 09 | 3 | ENG | @0 Thickness @5 09 |
---|
C03 | 10 | 3 | FRE | @0 Etude expérimentale @5 10 |
---|
C03 | 10 | 3 | ENG | @0 Experimental study @5 10 |
---|
C03 | 11 | 3 | FRE | @0 Oscillation @5 11 |
---|
C03 | 11 | 3 | ENG | @0 Oscillations @5 11 |
---|
C03 | 12 | X | FRE | @0 Préparation @5 12 |
---|
C03 | 12 | X | ENG | @0 Preparation @5 12 |
---|
C03 | 12 | X | GER | @0 Vorbereitung @5 12 |
---|
C03 | 12 | X | SPA | @0 Preparación @5 12 |
---|
C03 | 13 | X | FRE | @0 Pulvérisation haute fréquence @5 13 |
---|
C03 | 13 | X | ENG | @0 Radiofrequency sputtering @5 13 |
---|
C03 | 13 | X | SPA | @0 Pulverización alta frecuencia @5 13 |
---|
C03 | 14 | 3 | FRE | @0 Cobalt @2 NC @5 14 |
---|
C03 | 14 | 3 | ENG | @0 Cobalt @2 NC @5 14 |
---|
C03 | 15 | 3 | FRE | @0 Cuivre @2 NC @5 15 |
---|
C03 | 15 | 3 | ENG | @0 Copper @2 NC @5 15 |
---|
C03 | 16 | 3 | FRE | @0 7570P @2 PAC @4 INC @5 56 |
---|
C03 | 17 | 3 | FRE | @0 6835C @2 PAC @4 INC @5 57 |
---|
C03 | 18 | 3 | FRE | @0 Co @4 INC @5 92 |
---|
C03 | 19 | 3 | FRE | @0 Cu @4 INC @5 93 |
---|
C07 | 01 | 3 | FRE | @0 Métal transition @5 16 |
---|
C07 | 01 | 3 | ENG | @0 Transition elements @5 16 |
---|
N21 | | | | @1 069 |
---|
|
pR |
A30 | 01 | 1 | ENG | @1 EMRS-E : EMRS-E Symp. Magn. Ultrahin Films, Multilayers & Surfaces @3 Strasbourg @4 1996-06-07 |
---|
|
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Le document en format XML
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<term>Giant magnetoresistance</term>
<term>Multilayers</term>
<term>Oscillations</term>
<term>Preparation</term>
<term>Radiofrequency sputtering</term>
<term>Roughness</term>
<term>Size effect</term>
<term>Solid-solid interfaces</term>
<term>Texture</term>
<term>Thickness</term>
<term>XRD</term>
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<keywords scheme="Pascal" xml:lang="fr"><term>Magnétorésistance géante</term>
<term>Texture</term>
<term>Rugosité</term>
<term>Interface solide solide</term>
<term>Multicouche</term>
<term>XRD</term>
<term>Résonance antiferromagnétique</term>
<term>Effet dimensionnel</term>
<term>Epaisseur</term>
<term>Etude expérimentale</term>
<term>Oscillation</term>
<term>Préparation</term>
<term>Pulvérisation haute fréquence</term>
<term>Cobalt</term>
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<front><div type="abstract" xml:lang="en">Copyright (c) 1996 Elsevier Science B.V. All rights reserved. The objectives of the present work were two fold: first to obtain the highest giant magnetoresistance (GMR) ratio in Co/Cu multilayers grown from the unusual process of rf diode sputtering and second, to investigate in detail correlation between GMR and texture and the interfacial roughness deduced from X-ray diffraction and AFM, respectively. Different interface structures have been induced from the change of the sputtering parameters (sputtering argon gas pressure P<sub>Ar</sub>
) which gave the optimal rf sputtering conditions for high GMR. From different results it is concluded that the most important parameter is interface roughness which induces a strong effect on both the GMR and the resistivity of the superlattice. A change in the t<sub>Co</sub>
<sup>2</sup>
dependence of the reciprocal resistance near t<sub>Co</sub>
=25 Å is attributed to an increase of the effect of the layer roughness when the t<sub>Co</sub>
is going from mesoscopic (t<sub>Co</sub>
>25 Å) to nanoscopic scale (t<sub>Co</sub>
<25 Å).</div>
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<fA64 i1="01" i2="1"><s0>Journal of magnetism and magnetic materials</s0>
</fA64>
<fA66 i1="01"><s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Copyright (c) 1996 Elsevier Science B.V. All rights reserved. The objectives of the present work were two fold: first to obtain the highest giant magnetoresistance (GMR) ratio in Co/Cu multilayers grown from the unusual process of rf diode sputtering and second, to investigate in detail correlation between GMR and texture and the interfacial roughness deduced from X-ray diffraction and AFM, respectively. Different interface structures have been induced from the change of the sputtering parameters (sputtering argon gas pressure P<sub>Ar</sub>
) which gave the optimal rf sputtering conditions for high GMR. From different results it is concluded that the most important parameter is interface roughness which induces a strong effect on both the GMR and the resistivity of the superlattice. A change in the t<sub>Co</sub>
<sup>2</sup>
dependence of the reciprocal resistance near t<sub>Co</sub>
=25 Å is attributed to an increase of the effect of the layer roughness when the t<sub>Co</sub>
is going from mesoscopic (t<sub>Co</sub>
>25 Å) to nanoscopic scale (t<sub>Co</sub>
<25 Å).</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E70P</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B60H35C</s0>
</fC02>
<fC02 i1="03" i2="X"><s0>240</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Magnétorésistance géante</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Giant magnetoresistance</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Texture</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Texture</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Rugosité</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Roughness</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Interface solide solide</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Solid-solid interfaces</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Multicouche</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Multilayers</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>XRD</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>XRD</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Résonance antiferromagnétique</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Antiferromagnetic resonance</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Effet dimensionnel</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Size effect</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Epaisseur</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Thickness</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Oscillation</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Oscillations</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Préparation</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Preparation</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="GER"><s0>Vorbereitung</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Preparación</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Pulvérisation haute fréquence</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Radiofrequency sputtering</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Pulverización alta frecuencia</s0>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Cuivre</s0>
<s2>NC</s2>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Copper</s0>
<s2>NC</s2>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>7570P</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>6835C</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Co</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Cu</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Métal transition</s0>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Transition elements</s0>
<s5>16</s5>
</fC07>
<fN21><s1>069</s1>
</fN21>
</pA>
<pR><fA30 i1="01" i2="1" l="ENG"><s1>EMRS-E : EMRS-E Symp. Magn. Ultrahin Films, Multilayers & Surfaces</s1>
<s3>Strasbourg</s3>
<s4>1996-06-07</s4>
</fA30>
</pR>
</standard>
</inist>
</record>
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