CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000044

Random anisotropy model approach on ion beam sputtered Co20Cu80 granular alloy

Identifieur interne : 000044 ( PascalFrancis/Curation ); précédent : 000043; suivant : 000045

Random anisotropy model approach on ion beam sputtered Co20Cu80 granular alloy

Auteurs : H. Errahmani [Maroc] ; N. Hassanaïn [Maroc] ; A. Berrada [Maroc] ; M. Abid [Maroc] ; H. Lassri [Maroc] ; G. Schmerber [France] ; A. Dinia [France]

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2002.

RBID : Pascal:02-0366182

Descripteurs français

Pascal (Inist)
- Effet aléatoire, Anisotropie magnétique, Faisceau ion, Pulvérisation faisceau ionique, Propriété magnétique, Dépendance température, Onde spin, Rigidité, Interaction échange, Longueur corrélation, Grosseur grain, Microscopie électronique transmission, Cuivre alliage, Cobalt alliage, Alliage binaire, Alliage CoCu, Co Cu, Co20Cu80, 7540G, 7530G.

English descriptors

KwdEn :
- Binary alloys, Cobalt alloys, Copper alloys, Correlation length, Exchange interactions, Grain size, Ion beam sputtering, Ion beams, Magnetic anisotropy, Magnetic properties, Random effect, Spin waves, Stiffness, Temperature dependence, Transmission electron microscopy.

Abstract

The Co₂₀Cu₈₀ granular film has been elaborated using ion beam sputtering technique. The magnetic properties of the sample were studied in the temperature range 5-300 K at H ≤ 50 kOe. From the thermomagnetisation curve, which is found to obey to the Bloch law, we have extracted the spin wave stiffness constant D and the exchange constant A. The magnetic experimental results have been interpreted in the framework of random anisotropy model. We have determined the local anisotropy constant K_L and the local correlation length of anisotropy axis R_a, which is compared to the experimental grains size obtained by transmission electronic microscopy.

A01	`01`	`1`		`@0 0304-8853`
A02	`01`			`@0 JMMMDC`
A03		`1`		`@0 J. magn. magn. mater.`
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A08	`01`	`1`	`ENG`	`@1 Random anisotropy model approach on ion beam sputtered Co₂₀Cu₈₀ granular alloy`
A11	`01`	`1`		`@1 ERRAHMANI (H.)`
A11	`02`	`1`		`@1 HASSANAÏN (N.)`
A11	`03`	`1`		`@1 BERRADA (A.)`
A11	`04`	`1`		`@1 ABID (M.)`
A11	`05`	`1`		`@1 LASSRI (H.)`
A11	`06`	`1`		`@1 SCHMERBER (G.)`
A11	`07`	`1`		`@1 DINIA (A.)`
A14	`01`			`@1 L. P. M, Département de physique, Faculté des Sciences, B.P 1014 @2 Rabat @3 MAR @Z 1 aut. @Z 2 aut. @Z 3 aut.`
A14	`02`			`@1 L. P. M, Département de physique, Faculté des Sciences, Ain Chock B.P. 5356 @2 Casablanca @3 MAR @Z 4 aut. @Z 5 aut.`
A14	`03`			`@1 IPCMS-GEMM (7504, CNRS), ULP-ECPM, 23 rue du Loess @2 67037 Strasbourg @3 FRA @Z 6 aut. @Z 7 aut.`
A20				`@1 335-339`
A21				`@1 2002`
A23	`01`			`@0 ENG`
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A44				`@0 0000 @1 © 2002 INIST-CNRS. All rights reserved.`
A45				`@0 21 ref.`
A47	`01`	`1`		`@0 02-0366182`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of magnetism and magnetic materials`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 The Co₂₀Cu₈₀ granular film has been elaborated using ion beam sputtering technique. The magnetic properties of the sample were studied in the temperature range 5-300 K at H ≤ 50 kOe. From the thermomagnetisation curve, which is found to obey to the Bloch law, we have extracted the spin wave stiffness constant D and the exchange constant A. The magnetic experimental results have been interpreted in the framework of random anisotropy model. We have determined the local anisotropy constant K_L and the local correlation length of anisotropy axis R_a, which is compared to the experimental grains size obtained by transmission electronic microscopy.
C02	`01`	`3`		`@0 001B70E40G`
C02	`02`	`3`		`@0 001B70E30G`
C03	`01`	`X`	`FRE`	`@0 Effet aléatoire @5 02`
C03	`01`	`X`	`ENG`	`@0 Random effect @5 02`
C03	`01`	`X`	`SPA`	`@0 Efecto aleatorio @5 02`
C03	`02`	`3`	`FRE`	`@0 Anisotropie magnétique @5 03`
C03	`02`	`3`	`ENG`	`@0 Magnetic anisotropy @5 03`
C03	`03`	`3`	`FRE`	`@0 Faisceau ion @5 04`
C03	`03`	`3`	`ENG`	`@0 Ion beams @5 04`
C03	`04`	`X`	`FRE`	`@0 Pulvérisation faisceau ionique @5 05`
C03	`04`	`X`	`ENG`	`@0 Ion beam sputtering @5 05`
C03	`04`	`X`	`SPA`	`@0 Pulverización haz iónico @5 05`
C03	`05`	`3`	`FRE`	`@0 Propriété magnétique @5 06`
C03	`05`	`3`	`ENG`	`@0 Magnetic properties @5 06`
C03	`06`	`3`	`FRE`	`@0 Dépendance température @5 07`
C03	`06`	`3`	`ENG`	`@0 Temperature dependence @5 07`
C03	`07`	`3`	`FRE`	`@0 Onde spin @5 08`
C03	`07`	`3`	`ENG`	`@0 Spin waves @5 08`
C03	`08`	`X`	`FRE`	`@0 Rigidité @5 09`
C03	`08`	`X`	`ENG`	`@0 Stiffness @5 09`
C03	`08`	`X`	`SPA`	`@0 Rigidez @5 09`
C03	`09`	`3`	`FRE`	`@0 Interaction échange @5 10`
C03	`09`	`3`	`ENG`	`@0 Exchange interactions @5 10`
C03	`10`	`3`	`FRE`	`@0 Longueur corrélation @5 11`
C03	`10`	`3`	`ENG`	`@0 Correlation length @5 11`
C03	`11`	`3`	`FRE`	`@0 Grosseur grain @5 12`
C03	`11`	`3`	`ENG`	`@0 Grain size @5 12`
C03	`12`	`3`	`FRE`	`@0 Microscopie électronique transmission @5 13`
C03	`12`	`3`	`ENG`	`@0 Transmission electron microscopy @5 13`
C03	`13`	`3`	`FRE`	`@0 Cuivre alliage @5 15`
C03	`13`	`3`	`ENG`	`@0 Copper alloys @5 15`
C03	`14`	`3`	`FRE`	`@0 Cobalt alliage @5 16`
C03	`14`	`3`	`ENG`	`@0 Cobalt alloys @5 16`
C03	`15`	`3`	`FRE`	`@0 Alliage binaire @5 17`
C03	`15`	`3`	`ENG`	`@0 Binary alloys @5 17`
C03	`16`	`3`	`FRE`	`@0 Alliage CoCu @4 INC @5 52`
C03	`17`	`3`	`FRE`	`@0 Co Cu @4 INC @5 53`
C03	`18`	`3`	`FRE`	`@0 Co20Cu80 @4 INC @5 54`
C03	`19`	`3`	`FRE`	`@0 7540G @2 PAC @4 INC @5 56`
C03	`20`	`3`	`FRE`	`@0 7530G @2 PAC @4 INC @5 57`
C07	`01`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C07	`01`	`3`	`ENG`	`@0 Transition element alloys @5 48`
C07	`02`	`3`	`FRE`	`@0 Composé minéral @5 49`
C07	`02`	`3`	`ENG`	`@0 Inorganic compounds @5 49`
N21				`@1 203`
N82				`@1 PSI`

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Pascal:02-0366182

Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Random anisotropy model approach on ion beam sputtered Co<sub>20</sub>
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<term>Correlation length</term>
<term>Exchange interactions</term>
<term>Grain size</term>
<term>Ion beam sputtering</term>
<term>Ion beams</term>
<term>Magnetic anisotropy</term>
<term>Magnetic properties</term>
<term>Random effect</term>
<term>Spin waves</term>
<term>Stiffness</term>
<term>Temperature dependence</term>
<term>Transmission electron microscopy</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Effet aléatoire</term>
<term>Anisotropie magnétique</term>
<term>Faisceau ion</term>
<term>Pulvérisation faisceau ionique</term>
<term>Propriété magnétique</term>
<term>Dépendance température</term>
<term>Onde spin</term>
<term>Rigidité</term>
<term>Interaction échange</term>
<term>Longueur corrélation</term>
<term>Grosseur grain</term>
<term>Microscopie électronique transmission</term>
<term>Cuivre alliage</term>
<term>Cobalt alliage</term>
<term>Alliage binaire</term>
<term>Alliage CoCu</term>
<term>Co Cu</term>
<term>Co20Cu80</term>
<term>7540G</term>
<term>7530G</term>
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<front><div type="abstract" xml:lang="en">The Co<sub>20</sub>
Cu<sub>80</sub>
 granular film has been elaborated using ion beam sputtering technique. The magnetic properties of the sample were studied in the temperature range 5-300 K at H ≤ 50 kOe. From the thermomagnetisation curve, which is found to obey to the Bloch law, we have extracted the spin wave stiffness constant D and the exchange constant A. The magnetic experimental results have been interpreted in the framework of random anisotropy model. We have determined the local anisotropy constant K<sub>L</sub>
 and the local correlation length of anisotropy axis R<sub>a</sub>
, which is compared to the experimental grains size obtained by transmission electronic microscopy.</div>
</front>
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Cu<sub>80</sub>
 granular alloy</s1>
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<fA11 i1="01" i2="1"><s1>ERRAHMANI (H.)</s1>
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<fA14 i1="01"><s1>L. P. M, Département de physique, Faculté des Sciences, B.P 1014</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<fA14 i1="02"><s1>L. P. M, Département de physique, Faculté des Sciences, Ain Chock B.P. 5356</s1>
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<s3>MAR</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
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<fA14 i1="03"><s1>IPCMS-GEMM (7504, CNRS), ULP-ECPM, 23 rue du Loess</s1>
<s2>67037 Strasbourg</s2>
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<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
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</fA66>
<fC01 i1="01" l="ENG"><s0>The Co<sub>20</sub>
Cu<sub>80</sub>
 granular film has been elaborated using ion beam sputtering technique. The magnetic properties of the sample were studied in the temperature range 5-300 K at H ≤ 50 kOe. From the thermomagnetisation curve, which is found to obey to the Bloch law, we have extracted the spin wave stiffness constant D and the exchange constant A. The magnetic experimental results have been interpreted in the framework of random anisotropy model. We have determined the local anisotropy constant K<sub>L</sub>
 and the local correlation length of anisotropy axis R<sub>a</sub>
, which is compared to the experimental grains size obtained by transmission electronic microscopy.</s0>
</fC01>
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<s5>02</s5>
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<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Magnetic anisotropy</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Faisceau ion</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Ion beams</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Pulvérisation faisceau ionique</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Ion beam sputtering</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Pulverización haz iónico</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Propriété magnétique</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Magnetic properties</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="3" l="FRE"><s0>Onde spin</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Spin waves</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Rigidité</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Stiffness</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Rigidez</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Interaction échange</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Exchange interactions</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Longueur corrélation</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Correlation length</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Grosseur grain</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Grain size</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Microscopie électronique transmission</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Transmission electron microscopy</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Cuivre alliage</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Copper alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Cobalt alliage</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Cobalt alloys</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Alliage binaire</s0>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Binary alloys</s0>
<s5>17</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Alliage CoCu</s0>
<s4>INC</s4>
<s5>52</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Co Cu</s0>
<s4>INC</s4>
<s5>53</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Co20Cu80</s0>
<s4>INC</s4>
<s5>54</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>7540G</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>7530G</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>48</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>48</s5>
</fC07>
<fC07 i1="02" i2="3" l="FRE"><s0>Composé minéral</s0>
<s5>49</s5>
</fC07>
<fC07 i1="02" i2="3" l="ENG"><s0>Inorganic compounds</s0>
<s5>49</s5>
</fC07>
<fN21><s1>203</s1>
</fN21>
<fN82><s1>PSI</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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Random anisotropy model approach on ion beam sputtered Co20Cu80 granular alloy

Random anisotropy model approach on ion beam sputtered Co20Cu80 granular alloy

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