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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 :

RBID : Pascal:97-0157111

Descripteurs français

English descriptors

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
A11 01  1    @1 BEN YOUSSEF (J.)
A11 02  1    @1 BOUZIANE (K.)
A11 03  1    @1 KOSHKINA (O.)
A11 04  1    @1 LE GALL (H.)
A11 05  1    @1 EL HARFAOUI (M.)
A11 06  1    @1 EL YAMANI (M.)
A11 07  1    @1 DESVIGNES (J. M.)
A11 08  1    @1 FERT (A.)
A14 01      @2 92195 Meudon-Bellevue @3 FRA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 7 aut.
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A20       @1 288-291
A21       @1 1997
A23 01      @0 ENG
A24 01      @0 eng
A43 01      @1 INIST @2 17230 @5 354000063124420138
A44       @0 9000 @1 © 1997 Elsevier Science B.V. All rights reserved.
A47 01  1    @0 97-0157111
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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&rpar; 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&rpar; 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 &Aring; is attributed to an increase of the effect of the layer roughness when the tCo is going from mesoscopic (tCo>25 &Aring;&rpar; to nanoscopic scale (tCo<25 &Aring;&rpar;.
C02 01  3    @0 001B70E70P
C02 02  3    @0 001B60H35C
C02 03  X    @0 240
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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<term>Giant magnetoresistance</term>
<term>Multilayers</term>
<term>Oscillations</term>
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<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
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<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
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<sub>Co</sub>
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<sub>Co</sub>
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</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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