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Magnetic properties in amorphous Co93-XTbxZr7 thin films

Identifieur interne : 000388 ( PascalFrancis/Curation ); précédent : 000387; suivant : 000389

Magnetic properties in amorphous Co93-XTbxZr7 thin films

Auteurs : H. Ouahmane [Maroc] ; H. Lassri [Maroc] ; A. Itri [Maroc] ; A. Khmou [Maroc] ; G. Suran [France]

Source :

RBID : Pascal:98-0411684

Descripteurs français

English descriptors

Abstract

Amorphous Co93-xTbXZr7 thin films with a well-defined in-plane uniaxial anisotropy were prepared by RF sputtering. The saturation magnetization 4πMs, the uniaxial anisotropy constant Ku and the coercive field Hc were studied as a function of temperature and for the composition range 0 < X < 7. The Tb moment at 4.2 K is found to be 9μB in agreement with the theoretical value. This would indicate a collinear spin structure for Tb. The mean-field theory has been used to explain the temperature dependence of the magnetization. The exchange interactions between Co-Co and Co-Tb atom pairs have been evaluated. Ku and Hc are related by the equation Hc = αKun/μ0Ms with the fitting parameters α and n.
pA  
A01 01  1    @0 0921-4526
A03   1    @0 Physica, B Condens. matter
A05       @2 253
A06       @2 1-2
A08 01  1  ENG  @1 Magnetic properties in amorphous Co93-XTbxZr7 thin films
A11 01  1    @1 OUAHMANE (H.)
A11 02  1    @1 LASSRI (H.)
A11 03  1    @1 ITRI (A.)
A11 04  1    @1 KHMOU (A.)
A11 05  1    @1 SURAN (G.)
A14 01      @1 Département de physique, Université Moulay Ismaïl, Faculté des sciences et techniques, d'Errachidia, Boutalamine B.P. 509 Errachidia @3 MAR @Z 1 aut.
A14 02      @1 LPS, Université Moulay Ismail, Faculté des sciences de Meknes, B.P. 4010 @3 MAR @Z 1 aut. @Z 4 aut.
A14 03      @1 LPMME, Université Hassan II, Faculté des sciences Ain chok, Maârif, B.P. 5366, Route d'El Jadida, km 8 @2 Casablanca @3 MAR @Z 2 aut.
A14 04      @1 LPM, Université Mohammed V, Faculté des sciences, avenue Ibn Batouta, B.P. 1014 @2 Rabat @3 MAR @Z 3 aut.
A14 05      @1 Laboratoire de Magnetisme de Louis. Néel, CNRS, Av. des Marthyrs B.P. @2 38042 38 Grenoble @3 FRA @Z 5 aut.
A20       @1 142-147
A21       @1 1998
A23 01      @0 ENG
A43 01      @1 INIST @2 145B @5 354000072855220200
A44       @0 0000 @1 © 1998 INIST-CNRS. All rights reserved.
A45       @0 21 ref.
A47 01  1    @0 98-0411684
A60       @1 P
A61       @0 A
A64   1    @0 Physica. B, Condensed matter
A66 01      @0 NLD
C01 01    ENG  @0 Amorphous Co93-xTbXZr7 thin films with a well-defined in-plane uniaxial anisotropy were prepared by RF sputtering. The saturation magnetization 4πMs, the uniaxial anisotropy constant Ku and the coercive field Hc were studied as a function of temperature and for the composition range 0 < X < 7. The Tb moment at 4.2 K is found to be 9μB in agreement with the theoretical value. This would indicate a collinear spin structure for Tb. The mean-field theory has been used to explain the temperature dependence of the magnetization. The exchange interactions between Co-Co and Co-Tb atom pairs have been evaluated. Ku and Hc are related by the equation Hc = αKun/μ0Ms with the fitting parameters α and n.
C02 01  3    @0 001B70E70A
C02 02  X    @0 240
C03 01  3  FRE  @0 Etude expérimentale @5 01
C03 01  3  ENG  @0 Experimental study @5 01
C03 02  3  FRE  @0 Etat amorphe @5 02
C03 02  3  ENG  @0 Amorphous state @5 02
C03 03  3  FRE  @0 Couche mince @5 03
C03 03  3  ENG  @0 Thin films @5 03
C03 04  3  FRE  @0 Anisotropie magnétique @5 05
C03 04  3  ENG  @0 Magnetic anisotropy @5 05
C03 05  3  FRE  @0 Théorie champ moyen @5 06
C03 05  3  ENG  @0 Mean-field theory @5 06
C03 06  3  FRE  @0 Dépendance température @5 07
C03 06  3  ENG  @0 Temperature dependence @5 07
C03 07  X  FRE  @0 Aimantation saturation @5 08
C03 07  X  ENG  @0 Saturation magnetization @5 08
C03 07  X  SPA  @0 Imanación saturación @5 08
C03 08  3  FRE  @0 Interaction échange @5 09
C03 08  3  ENG  @0 Exchange interactions @5 09
C03 09  3  FRE  @0 Force coercitive @5 10
C03 09  3  ENG  @0 Coercive force @5 10
C03 10  3  FRE  @0 Structure magnétique @5 11
C03 10  3  ENG  @0 Magnetic structure @5 11
C03 11  3  FRE  @0 Effet concentration @5 12
C03 11  3  ENG  @0 Quantity ratio @5 12
C03 12  3  FRE  @0 Alliage base cobalt @2 NK @5 13
C03 12  3  ENG  @0 Cobalt base alloys @2 NK @5 13
C03 13  3  FRE  @0 Terbium alliage @5 14
C03 13  3  ENG  @0 Terbium alloys @5 14
C03 14  3  FRE  @0 Zirconium alliage @5 15
C03 14  3  ENG  @0 Zirconium alloys @5 15
C03 15  3  FRE  @0 Alliage ternaire @5 16
C03 15  3  ENG  @0 Ternary alloys @5 16
C03 16  3  FRE  @0 7570A @2 PAC @4 INC @5 56
C03 17  3  FRE  @0 Alliage CoTbZr @2 NK @4 INC @5 92
C03 18  3  FRE  @0 Co Tb Zr @4 INC @5 93
C07 01  3  FRE  @0 Métal transition alliage @5 17
C07 01  3  ENG  @0 Transition element alloys @5 17
C07 02  3  FRE  @0 Lanthanide alliage @5 81
C07 02  3  ENG  @0 Rare earth alloys @5 81
N21       @1 278

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<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
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</affiliation>
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<term>Exchange interactions</term>
<term>Experimental study</term>
<term>Magnetic anisotropy</term>
<term>Magnetic structure</term>
<term>Mean-field theory</term>
<term>Quantity ratio</term>
<term>Saturation magnetization</term>
<term>Temperature dependence</term>
<term>Terbium alloys</term>
<term>Ternary alloys</term>
<term>Thin films</term>
<term>Zirconium alloys</term>
</keywords>
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<term>Etude expérimentale</term>
<term>Etat amorphe</term>
<term>Couche mince</term>
<term>Anisotropie magnétique</term>
<term>Théorie champ moyen</term>
<term>Dépendance température</term>
<term>Aimantation saturation</term>
<term>Interaction échange</term>
<term>Force coercitive</term>
<term>Structure magnétique</term>
<term>Effet concentration</term>
<term>Alliage base cobalt</term>
<term>Terbium alliage</term>
<term>Zirconium alliage</term>
<term>Alliage ternaire</term>
<term>7570A</term>
<term>Alliage CoTbZr</term>
<term>Co Tb Zr</term>
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<div type="abstract" xml:lang="en">Amorphous Co
<sub>93-x</sub>
Tb
<sub>X</sub>
Zr
<sub>7</sub>
thin films with a well-defined in-plane uniaxial anisotropy were prepared by RF sputtering. The saturation magnetization 4πM
<sub>s</sub>
, the uniaxial anisotropy constant K
<sub>u</sub>
and the coercive field H
<sub>c</sub>
were studied as a function of temperature and for the composition range 0 < X < 7. The Tb moment at 4.2 K is found to be 9μ
<sub>B</sub>
in agreement with the theoretical value. This would indicate a collinear spin structure for Tb. The mean-field theory has been used to explain the temperature dependence of the magnetization. The exchange interactions between Co-Co and Co-Tb atom pairs have been evaluated. K
<sub>u</sub>
and H
<sub>c</sub>
are related by the equation H
<sub>c</sub>
= αK
<sub>un/μ0</sub>
M
<sub>s</sub>
with the fitting parameters α and n.</div>
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<s1>Magnetic properties in amorphous Co
<sub>93-X</sub>
TbxZr
<sub>7</sub>
thin films</s1>
</fA08>
<fA11 i1="01" i2="1">
<s1>OUAHMANE (H.)</s1>
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<s1>SURAN (G.)</s1>
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<s1>Département de physique, Université Moulay Ismaïl, Faculté des sciences et techniques, d'Errachidia, Boutalamine B.P. 509 Errachidia</s1>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
</fA14>
<fA14 i1="02">
<s1>LPS, Université Moulay Ismail, Faculté des sciences de Meknes, B.P. 4010</s1>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="03">
<s1>LPMME, Université Hassan II, Faculté des sciences Ain chok, Maârif, B.P. 5366, Route d'El Jadida, km 8</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="04">
<s1>LPM, Université Mohammed V, Faculté des sciences, avenue Ibn Batouta, B.P. 1014</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="05">
<s1>Laboratoire de Magnetisme de Louis. Néel, CNRS, Av. des Marthyrs B.P.</s1>
<s2>38042 38 Grenoble</s2>
<s3>FRA</s3>
<sZ>5 aut.</sZ>
</fA14>
<fA20>
<s1>142-147</s1>
</fA20>
<fA21>
<s1>1998</s1>
</fA21>
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</fA23>
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<s5>354000072855220200</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 1998 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>21 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>98-0411684</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
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<s0>A</s0>
</fA61>
<fA64 i2="1">
<s0>Physica. B, Condensed matter</s0>
</fA64>
<fA66 i1="01">
<s0>NLD</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>Amorphous Co
<sub>93-x</sub>
Tb
<sub>X</sub>
Zr
<sub>7</sub>
thin films with a well-defined in-plane uniaxial anisotropy were prepared by RF sputtering. The saturation magnetization 4πM
<sub>s</sub>
, the uniaxial anisotropy constant K
<sub>u</sub>
and the coercive field H
<sub>c</sub>
were studied as a function of temperature and for the composition range 0 < X < 7. The Tb moment at 4.2 K is found to be 9μ
<sub>B</sub>
in agreement with the theoretical value. This would indicate a collinear spin structure for Tb. The mean-field theory has been used to explain the temperature dependence of the magnetization. The exchange interactions between Co-Co and Co-Tb atom pairs have been evaluated. K
<sub>u</sub>
and H
<sub>c</sub>
are related by the equation H
<sub>c</sub>
= αK
<sub>un/μ0</sub>
M
<sub>s</sub>
with the fitting parameters α and n.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001B70E70A</s0>
</fC02>
<fC02 i1="02" i2="X">
<s0>240</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Etude expérimentale</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Experimental study</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE">
<s0>Etat amorphe</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Amorphous state</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Couche mince</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Thin films</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Anisotropie magnétique</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Magnetic anisotropy</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Théorie champ moyen</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Mean-field theory</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Dépendance température</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG">
<s0>Temperature dependence</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE">
<s0>Aimantation saturation</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG">
<s0>Saturation magnetization</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA">
<s0>Imanación saturación</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Interaction échange</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Exchange interactions</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Force coercitive</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Coercive force</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Structure magnétique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Magnetic structure</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Effet concentration</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Quantity ratio</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Alliage base cobalt</s0>
<s2>NK</s2>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Cobalt base alloys</s0>
<s2>NK</s2>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Terbium alliage</s0>
<s5>14</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Terbium alloys</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Zirconium alliage</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Zirconium alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Alliage ternaire</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Ternary alloys</s0>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>7570A</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Alliage CoTbZr</s0>
<s2>NK</s2>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE">
<s0>Co Tb Zr</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE">
<s0>Métal transition alliage</s0>
<s5>17</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG">
<s0>Transition element alloys</s0>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="3" l="FRE">
<s0>Lanthanide alliage</s0>
<s5>81</s5>
</fC07>
<fC07 i1="02" i2="3" l="ENG">
<s0>Rare earth alloys</s0>
<s5>81</s5>
</fC07>
<fN21>
<s1>278</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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