CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000393

Magnetic and magneto-optical studies in Co-Tb/Pt multilayers

Identifieur interne : 000393 ( PascalFrancis/Curation ); précédent : 000392; suivant : 000394

Magnetic and magneto-optical studies in Co-Tb/Pt multilayers

Auteurs : H. Hamouda [Maroc] ; H. Lassri [Maroc] ; R. Krishnan [France] ; D. Saifaoui [Maroc]

Source :

Solid state communications [ 0038-1098 ] ; 1998.

RBID : Pascal:98-0509397

Descripteurs français

Pascal (Inist)
- Etude expérimentale, Multicouche, Effet Kerr magnétooptique, Aimantation saturation, Force coercitive, Superréseau, Anisotropie magnétique, Hystérésis magnétique, Cobalt alliage, Terbium alliage, Platine, Alliage binaire, 7570C, Alliage CoTb, Pt, Co Tb.
Wicri :
- topic : Platine.

English descriptors

KwdEn :
- Binary alloys, Cobalt alloys, Coercive force, Experimental study, Kerr magneto-optical effect, Magnetic anisotropy, Magnetic hysteresis, Multilayers, Platinum, Saturation magnetization, Superlattices, Terbium alloys.

Abstract

We have prepared Co₈₆Tb₁₄/Pt multilayers by r.f. sputtering and studied their magnetic and magneto-optical properties. As the Co-Tb layer thickness (t_CoTb) decreases below 200A the saturation magnetization increases, the rectangularity of the M-H loops and the coercivity decrease. The effective anisotropy K_eff of the multilayers was determined by a torque magnetometer. The product K_eff X t_CoTb shows a linear dependence with t_CoTb as normally found for the superlattices yielding the bulk and surface anisotropies of 1 x 10 erg cm^-3 and - 0.2 erg cm^-2, respectively. These results are explained in terms of an interfacial Co-Pt layer. The polar Kerr rotation for the multilayers is found independent of layer thickness and is equal to 11.5 min, which is higher than the single thick layer.

A01	`01`	`1`		`@0 0038-1098`
A02	`01`			`@0 SSCOA4`
A03		`1`		`@0 Solid state commun.`
A05				`@2 108`
A06				`@2 7`
A08	`01`	`1`	`ENG`	`@1 Magnetic and magneto-optical studies in Co-Tb/Pt multilayers`
A11	`01`	`1`		`@1 HAMOUDA (H.)`
A11	`02`	`1`		`@1 LASSRI (H.)`
A11	`03`	`1`		`@1 KRISHNAN (R.)`
A11	`04`	`1`		`@1 SAIFAOUI (D.)`
A14	`01`			`@1 Laboratoire de Physique Théorique, Université Hassan II, Faculté des Sciences, B.P. 5366 Maârif, Ain Chock, Route d'El Jadida km-8 @2 Casablanca @3 MAR @Z 1 aut. @Z 4 aut.`
A14	`02`			`@1 Laboratoire de Physique des Matériaux et de Microélectronique, Université Hassan II, Faculté des Sciences, B.P.5366 Maârif, Ain Chock, Route d'El Jadida km-8 @2 Casablanca @3 MAR @Z 2 aut.`
A14	`03`			`@1 Laboratoire de Magnétisme et d'Optique de l'Université de Versailles, CNRS, URA 1531, 45, Avenue des Etats-Unis @2 78035 Versailles @3 FRA @Z 3 aut.`
A20				`@1 451-455`
A21				`@1 1998`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 10917 @5 354000071565740100`
A44				`@0 0000 @1 © 1998 INIST-CNRS. All rights reserved.`
A45				`@0 26 ref.`
A47	`01`	`1`		`@0 98-0509397`
A60				`@1 P`
A61				`@0 A`
A64		`1`		`@0 Solid state communications`
A66	`01`			`@0 USA`
C01	`01`		`ENG`	@0 We have prepared Co₈₆Tb₁₄/Pt multilayers by r.f. sputtering and studied their magnetic and magneto-optical properties. As the Co-Tb layer thickness (t_CoTb) decreases below 200A the saturation magnetization increases, the rectangularity of the M-H loops and the coercivity decrease. The effective anisotropy K_eff of the multilayers was determined by a torque magnetometer. The product K_eff X t_CoTb shows a linear dependence with t_CoTb as normally found for the superlattices yielding the bulk and surface anisotropies of 1 x 10 erg cm^-3 and - 0.2 erg cm^-2, respectively. These results are explained in terms of an interfacial Co-Pt layer. The polar Kerr rotation for the multilayers is found independent of layer thickness and is equal to 11.5 min, which is higher than the single thick layer.
C02	`01`	`3`		`@0 001B70E70C`
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 Multicouche @5 02`
C03	`02`	`3`	`ENG`	`@0 Multilayers @5 02`
C03	`03`	`3`	`FRE`	`@0 Effet Kerr magnétooptique @5 03`
C03	`03`	`3`	`ENG`	`@0 Kerr magneto-optical effect @5 03`
C03	`04`	`X`	`FRE`	`@0 Aimantation saturation @5 04`
C03	`04`	`X`	`ENG`	`@0 Saturation magnetization @5 04`
C03	`04`	`X`	`SPA`	`@0 Imanación saturación @5 04`
C03	`05`	`3`	`FRE`	`@0 Force coercitive @5 05`
C03	`05`	`3`	`ENG`	`@0 Coercive force @5 05`
C03	`06`	`3`	`FRE`	`@0 Superréseau @5 06`
C03	`06`	`3`	`ENG`	`@0 Superlattices @5 06`
C03	`07`	`3`	`FRE`	`@0 Anisotropie magnétique @5 07`
C03	`07`	`3`	`ENG`	`@0 Magnetic anisotropy @5 07`
C03	`08`	`3`	`FRE`	`@0 Hystérésis magnétique @5 08`
C03	`08`	`3`	`ENG`	`@0 Magnetic hysteresis @5 08`
C03	`09`	`3`	`FRE`	`@0 Cobalt alliage @5 12`
C03	`09`	`3`	`ENG`	`@0 Cobalt alloys @5 12`
C03	`10`	`3`	`FRE`	`@0 Terbium alliage @5 13`
C03	`10`	`3`	`ENG`	`@0 Terbium alloys @5 13`
C03	`11`	`3`	`FRE`	`@0 Platine @2 NC @5 14`
C03	`11`	`3`	`ENG`	`@0 Platinum @2 NC @5 14`
C03	`12`	`3`	`FRE`	`@0 Alliage binaire @5 15`
C03	`12`	`3`	`ENG`	`@0 Binary alloys @5 15`
C03	`13`	`3`	`FRE`	`@0 7570C @2 PAC @4 INC @5 56`
C03	`14`	`3`	`FRE`	`@0 Alliage CoTb @2 NK @4 INC @5 92`
C03	`15`	`3`	`FRE`	`@0 Pt @4 INC @5 93`
C03	`16`	`3`	`FRE`	`@0 Co Tb @4 INC @5 94`
C07	`01`	`3`	`FRE`	`@0 Métal transition alliage @5 16`
C07	`01`	`3`	`ENG`	`@0 Transition element alloys @5 16`
C07	`02`	`3`	`FRE`	`@0 Métal transition @5 17`
C07	`02`	`3`	`ENG`	`@0 Transition elements @5 17`
N21				`@1 334`

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetic and magneto-optical studies in Co-Tb/Pt multilayers</title>
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<s2>Casablanca</s2>
<s3>MAR</s3>
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<author><name sortKey="Lassri, H" sort="Lassri, H" uniqKey="Lassri H" first="H." last="Lassri">H. Lassri</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Laboratoire de Physique des Matériaux et de Microélectronique, Université Hassan II, Faculté des Sciences, B.P.5366 Maârif, Ain Chock, Route d'El Jadida km-8</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
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<author><name sortKey="Krishnan, R" sort="Krishnan, R" uniqKey="Krishnan R" first="R." last="Krishnan">R. Krishnan</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Laboratoire de Magnétisme et d'Optique de l'Université de Versailles, CNRS, URA 1531, 45, Avenue des Etats-Unis</s1>
<s2>78035 Versailles</s2>
<s3>FRA</s3>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>France</country>
</affiliation>
</author>
<author><name sortKey="Saifaoui, D" sort="Saifaoui, D" uniqKey="Saifaoui D" first="D." last="Saifaoui">D. Saifaoui</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Laboratoire de Physique Théorique, Université Hassan II, Faculté des Sciences, B.P. 5366 Maârif, Ain Chock, Route d'El Jadida km-8</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
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<country>Maroc</country>
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<series><title level="j" type="main">Solid state communications</title>
<title level="j" type="abbreviated">Solid state commun.</title>
<idno type="ISSN">0038-1098</idno>
<imprint><date when="1998">1998</date>
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<seriesStmt><title level="j" type="main">Solid state communications</title>
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</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Binary alloys</term>
<term>Cobalt alloys</term>
<term>Coercive force</term>
<term>Experimental study</term>
<term>Kerr magneto-optical effect</term>
<term>Magnetic anisotropy</term>
<term>Magnetic hysteresis</term>
<term>Multilayers</term>
<term>Platinum</term>
<term>Saturation magnetization</term>
<term>Superlattices</term>
<term>Terbium alloys</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude expérimentale</term>
<term>Multicouche</term>
<term>Effet Kerr magnétooptique</term>
<term>Aimantation saturation</term>
<term>Force coercitive</term>
<term>Superréseau</term>
<term>Anisotropie magnétique</term>
<term>Hystérésis magnétique</term>
<term>Cobalt alliage</term>
<term>Terbium alliage</term>
<term>Platine</term>
<term>Alliage binaire</term>
<term>7570C</term>
<term>Alliage CoTb</term>
<term>Pt</term>
<term>Co Tb</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Platine</term>
</keywords>
</textClass>
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<front><div type="abstract" xml:lang="en">We have prepared Co<sub>86</sub>
Tb<sub>14</sub>
/Pt multilayers by r.f. sputtering and studied their magnetic and magneto-optical properties. As the Co-Tb layer thickness (t<sub>CoTb</sub>
) decreases below 200A the saturation magnetization increases, the rectangularity of the M-H loops and the coercivity decrease. The effective anisotropy K<sub>eff</sub>
 of the multilayers was determined by a torque magnetometer. The product K<sub>eff</sub>
 X t<sub>CoTb</sub>
 shows a linear dependence with t<sub>CoTb</sub>
 as normally found for the superlattices yielding the bulk and surface anisotropies of 1 x 10 erg cm<sup>-3</sup>
 and - 0.2 erg cm<sup>-2</sup>
, respectively. These results are explained in terms of an interfacial Co-Pt layer. The polar Kerr rotation for the multilayers is found independent of layer thickness and is equal to 11.5 min, which is higher than the single thick layer.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Magnetic and magneto-optical studies in Co-Tb/Pt multilayers</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>HAMOUDA (H.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>LASSRI (H.)</s1>
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<fA11 i1="03" i2="1"><s1>KRISHNAN (R.)</s1>
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<fA11 i1="04" i2="1"><s1>SAIFAOUI (D.)</s1>
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<fA14 i1="01"><s1>Laboratoire de Physique Théorique, Université Hassan II, Faculté des Sciences, B.P. 5366 Maârif, Ain Chock, Route d'El Jadida km-8</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Laboratoire de Physique des Matériaux et de Microélectronique, Université Hassan II, Faculté des Sciences, B.P.5366 Maârif, Ain Chock, Route d'El Jadida km-8</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Laboratoire de Magnétisme et d'Optique de l'Université de Versailles, CNRS, URA 1531, 45, Avenue des Etats-Unis</s1>
<s2>78035 Versailles</s2>
<s3>FRA</s3>
<sZ>3 aut.</sZ>
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<fA20><s1>451-455</s1>
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<fC01 i1="01" l="ENG"><s0>We have prepared Co<sub>86</sub>
Tb<sub>14</sub>
/Pt multilayers by r.f. sputtering and studied their magnetic and magneto-optical properties. As the Co-Tb layer thickness (t<sub>CoTb</sub>
) decreases below 200A the saturation magnetization increases, the rectangularity of the M-H loops and the coercivity decrease. The effective anisotropy K<sub>eff</sub>
 of the multilayers was determined by a torque magnetometer. The product K<sub>eff</sub>
 X t<sub>CoTb</sub>
 shows a linear dependence with t<sub>CoTb</sub>
 as normally found for the superlattices yielding the bulk and surface anisotropies of 1 x 10 erg cm<sup>-3</sup>
 and - 0.2 erg cm<sup>-2</sup>
, respectively. These results are explained in terms of an interfacial Co-Pt layer. The polar Kerr rotation for the multilayers is found independent of layer thickness and is equal to 11.5 min, which is higher than the single thick layer.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E70C</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>Multicouche</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Multilayers</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Effet Kerr magnétooptique</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Kerr magneto-optical effect</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Aimantation saturation</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Saturation magnetization</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Imanación saturación</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Force coercitive</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Coercive force</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Superréseau</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Superlattices</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Anisotropie magnétique</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Magnetic anisotropy</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Hystérésis magnétique</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Magnetic hysteresis</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Cobalt alliage</s0>
<s5>12</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Cobalt alloys</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Terbium alliage</s0>
<s5>13</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Terbium alloys</s0>
<s5>13</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Platine</s0>
<s2>NC</s2>
<s5>14</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Platinum</s0>
<s2>NC</s2>
<s5>14</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Alliage binaire</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Binary alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>7570C</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Alliage CoTb</s0>
<s2>NK</s2>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Pt</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Co Tb</s0>
<s4>INC</s4>
<s5>94</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>16</s5>
</fC07>
<fC07 i1="02" i2="3" l="FRE"><s0>Métal transition</s0>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="3" l="ENG"><s0>Transition elements</s0>
<s5>17</s5>
</fC07>
<fN21><s1>334</s1>
</fN21>
</pA>
</standard>
</inist>
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	Serveur d'exploration sur le cobalt au Maghreb
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Serveur d'exploration sur le cobalt au Maghreb

Magnetic and magneto-optical studies in Co-Tb/Pt multilayers

Magnetic and magneto-optical studies in Co-Tb/Pt multilayers

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