Serveur d'exploration sur le cobalt au Maghreb

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Spin-Wave Excitations in Evaporated Co/Pt Multilayers

Identifieur interne : 000227 ( PascalFrancis/Curation ); précédent : 000226; suivant : 000228

Spin-Wave Excitations in Evaporated Co/Pt Multilayers

Auteurs : H. Salhi [Maroc] ; K. Chafai [Maroc] ; O. Msieh [Maroc] ; H. Lassri [Maroc] ; K. Benkirane [Maroc] ; M. Abid [Maroc] ; L. Bessais [France] ; E. K. Hlil [France]

Source :

RBID : Pascal:11-0378010

Descripteurs français

English descriptors

Abstract

The magnetic properties of evaporated Co/Pt multilayers have been studied by magnetic measurements and ferromagnetic resonance (FMR). The spin-wave resonances were observed in some multilayers in FMR experiments, which implied that spin waves were sustained by the whole and propagated through Pt layers. The relation of the resonance field Hres with the mode number n obeys the so-called n2 law and the interlayer coupling strength JI has been determined. The temperature dependence of the spontaneous magnetization can be well described by Bloch's law, in all multilayers. The increase of the spin-wave parameter B with decreasing cobalt thickness has been discussed. A spin-wave theory has been used to explain the temperature dependence of the magnetization and the approximate values for the bulk exchange interaction Jb and surface exchange interaction JS for various Co/Pt multilayers have been obtained.
pA  
A01 01  1    @0 1557-1939
A03   1    @0 J. supercond. nov. magn.
A05       @2 24
A06       @2 5
A08 01  1  ENG  @1 Spin-Wave Excitations in Evaporated Co/Pt Multilayers
A11 01  1    @1 SALHI (H.)
A11 02  1    @1 CHAFAI (K.)
A11 03  1    @1 MSIEH (O.)
A11 04  1    @1 LASSRI (H.)
A11 05  1    @1 BENKIRANE (K.)
A11 06  1    @1 ABID (M.)
A11 07  1    @1 BESSAIS (L.)
A11 08  1    @1 HLIL (E. K.)
A14 01      @1 Laboratoire de Physique des Matériaux, Micro-électronique, Automatique et Thermique, LPMMAT, Faculté des Sciences Ain Chock, Université Hassan II, B.P. 5366, Mâarif, Route d'El Jadida @2 km-8, Casablanca @3 MAR @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 6 aut.
A14 02      @1 Laboratoire de Mécanique, Productique et Genie Industriel, LMPG, Ecole supérieure de Technologie, Université Hassan II, B.P. 5366, Mâarif, Route d'El Jadida @2 km-8, Casablanca @3 MAR @Z 1 aut.
A14 03      @1 Ecole Royale Navale, Bd. Sour Jdid @2 Casablanca @3 MAR @Z 5 aut.
A14 04      @1 ICMPE-CMTR, UMR CNRS 7182, 2-8, rue H. Dunant @2 94320 Thiais @3 FRA @Z 7 aut.
A14 05      @1 Institut Néel, CNRS-Université J. Fourier, B.P. 166 @2 38042 Grenoble @3 FRA @Z 8 aut.
A20       @1 1375-1379
A21       @1 2011
A23 01      @0 ENG
A43 01      @1 INIST @2 21987 @5 354000508571440010
A44       @0 0000 @1 © 2011 INIST-CNRS. All rights reserved.
A45       @0 28 ref.
A47 01  1    @0 11-0378010
A60       @1 P
A61       @0 A
A64 01  1    @0 Journal of superconductivity and novel magnetism
A66 01      @0 USA
C01 01    ENG  @0 The magnetic properties of evaporated Co/Pt multilayers have been studied by magnetic measurements and ferromagnetic resonance (FMR). The spin-wave resonances were observed in some multilayers in FMR experiments, which implied that spin waves were sustained by the whole and propagated through Pt layers. The relation of the resonance field Hres with the mode number n obeys the so-called n2 law and the interlayer coupling strength JI has been determined. The temperature dependence of the spontaneous magnetization can be well described by Bloch's law, in all multilayers. The increase of the spin-wave parameter B with decreasing cobalt thickness has been discussed. A spin-wave theory has been used to explain the temperature dependence of the magnetization and the approximate values for the bulk exchange interaction Jb and surface exchange interaction JS for various Co/Pt multilayers have been obtained.
C02 01  3    @0 001B70E70C
C02 02  3    @0 001B70F50
C03 01  3  FRE  @0 Onde spin @5 02
C03 01  3  ENG  @0 Spin waves @5 02
C03 02  3  FRE  @0 Aimantation @5 03
C03 02  3  ENG  @0 Magnetization @5 03
C03 03  3  FRE  @0 Résonance ferromagnétique @5 04
C03 03  3  ENG  @0 Ferromagnetic resonance @5 04
C03 04  X  FRE  @0 Résonance onde spin @5 05
C03 04  X  ENG  @0 Spin wave resonance @5 05
C03 04  X  SPA  @0 Resonancia onda spin @5 05
C03 05  3  FRE  @0 Interaction échange @5 06
C03 05  3  ENG  @0 Exchange interactions @5 06
C03 06  3  FRE  @0 Aimantation spontanée @5 07
C03 06  3  ENG  @0 Spontaneous magnetization @5 07
C03 07  3  FRE  @0 Epaisseur @5 08
C03 07  3  ENG  @0 Thickness @5 08
C03 08  X  FRE  @0 Mesure magnétique @5 11
C03 08  X  ENG  @0 Magnetic measurement @5 11
C03 08  X  SPA  @0 Medida magnética @5 11
C03 09  3  FRE  @0 Multicouche @5 15
C03 09  3  ENG  @0 Multilayers @5 15
C03 10  3  FRE  @0 Cobalt @2 NC @5 16
C03 10  3  ENG  @0 Cobalt @2 NC @5 16
C03 11  3  FRE  @0 Platine @2 NC @5 17
C03 11  3  ENG  @0 Platinum @2 NC @5 17
C03 12  3  FRE  @0 Métal transition @5 48
C03 12  3  ENG  @0 Transition elements @5 48
N21       @1 262

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Pascal:11-0378010

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<term>Cobalt</term>
<term>Exchange interactions</term>
<term>Ferromagnetic resonance</term>
<term>Magnetic measurement</term>
<term>Magnetization</term>
<term>Multilayers</term>
<term>Platinum</term>
<term>Spin wave resonance</term>
<term>Spin waves</term>
<term>Spontaneous magnetization</term>
<term>Thickness</term>
<term>Transition elements</term>
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<term>Onde spin</term>
<term>Aimantation</term>
<term>Résonance ferromagnétique</term>
<term>Résonance onde spin</term>
<term>Interaction échange</term>
<term>Aimantation spontanée</term>
<term>Epaisseur</term>
<term>Mesure magnétique</term>
<term>Multicouche</term>
<term>Cobalt</term>
<term>Platine</term>
<term>Métal transition</term>
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<div type="abstract" xml:lang="en">The magnetic properties of evaporated Co/Pt multilayers have been studied by magnetic measurements and ferromagnetic resonance (FMR). The spin-wave resonances were observed in some multilayers in FMR experiments, which implied that spin waves were sustained by the whole and propagated through Pt layers. The relation of the resonance field H
<sub>res</sub>
with the mode number n obeys the so-called n
<sup>2</sup>
law and the interlayer coupling strength J
<sub>I</sub>
has been determined. The temperature dependence of the spontaneous magnetization can be well described by Bloch's law, in all multilayers. The increase of the spin-wave parameter B with decreasing cobalt thickness has been discussed. A spin-wave theory has been used to explain the temperature dependence of the magnetization and the approximate values for the bulk exchange interaction J
<sub>b</sub>
and surface exchange interaction J
<sub>S</sub>
for various Co/Pt multilayers have been obtained.</div>
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<fA14 i1="04">
<s1>ICMPE-CMTR, UMR CNRS 7182, 2-8, rue H. Dunant</s1>
<s2>94320 Thiais</s2>
<s3>FRA</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="05">
<s1>Institut Néel, CNRS-Université J. Fourier, B.P. 166</s1>
<s2>38042 Grenoble</s2>
<s3>FRA</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA20>
<s1>1375-1379</s1>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>21987</s2>
<s5>354000508571440010</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>28 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0378010</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Journal of superconductivity and novel magnetism</s0>
</fA64>
<fA66 i1="01">
<s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>The magnetic properties of evaporated Co/Pt multilayers have been studied by magnetic measurements and ferromagnetic resonance (FMR). The spin-wave resonances were observed in some multilayers in FMR experiments, which implied that spin waves were sustained by the whole and propagated through Pt layers. The relation of the resonance field H
<sub>res</sub>
with the mode number n obeys the so-called n
<sup>2</sup>
law and the interlayer coupling strength J
<sub>I</sub>
has been determined. The temperature dependence of the spontaneous magnetization can be well described by Bloch's law, in all multilayers. The increase of the spin-wave parameter B with decreasing cobalt thickness has been discussed. A spin-wave theory has been used to explain the temperature dependence of the magnetization and the approximate values for the bulk exchange interaction J
<sub>b</sub>
and surface exchange interaction J
<sub>S</sub>
for various Co/Pt multilayers have been obtained.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001B70E70C</s0>
</fC02>
<fC02 i1="02" i2="3">
<s0>001B70F50</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Onde spin</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Spin waves</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Aimantation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Magnetization</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Résonance ferromagnétique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Ferromagnetic resonance</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Résonance onde spin</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Spin wave resonance</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Resonancia onda spin</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Interaction échange</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Exchange interactions</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Aimantation spontanée</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG">
<s0>Spontaneous magnetization</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Epaisseur</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Thickness</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE">
<s0>Mesure magnétique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Magnetic measurement</s0>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Medida magnética</s0>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Multicouche</s0>
<s5>15</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Multilayers</s0>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Cobalt</s0>
<s2>NC</s2>
<s5>16</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Cobalt</s0>
<s2>NC</s2>
<s5>16</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Platine</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Platinum</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Métal transition</s0>
<s5>48</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Transition elements</s0>
<s5>48</s5>
</fC03>
<fN21>
<s1>262</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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