CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000141

Magnetic and structural properties of evaporated CoxCr1- x/Si(1 00) and CoxCr1- x/glass thin films

Identifieur interne : 000141 ( PascalFrancis/Curation ); précédent : 000140; suivant : 000142

Magnetic and structural properties of evaporated CoxCr1- x/Si(1 00) and CoxCr1- x/glass thin films

Auteurs : A. Kharmouche [Algérie] ; S.-M. Cherif [France] ; G. Schmerber [France] ; A. Bourzami [Algérie]

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2007.

RBID : Pascal:07-0052715

Descripteurs français

Pascal (Inist)
- Propriété magnétique, Evaporation sous vide, Epaisseur, Aimantation saturation, Force coercitive, Microscopie force magnétique, Structure domaine, Spectre Brillouin, Hystérésis magnétique, Domaine magnétique, Substrat, Chrome alliage, Couche mince, Réseau hexagonal compact, Cobalt alliage, Métal transition alliage, 7570C, 7570K, Domaine en rubans.

English descriptors

KwdEn :
- Brillouin spectra, Chromium alloys, Cobalt alloys, Coercive force, Domain structure, HCP lattices, Magnetic domains, Magnetic force microscopy, Magnetic hysteresis, Magnetic properties, Saturation magnetization, Stripe domains, Substrates, Thickness, Thin films, Transition element alloys, Vacuum evaporation.

Abstract

Series of Co_xCr_1-x thin films have been evaporated under vacuum onto Si(1 0 0) and glass substrates, where x variations were between 0.51 and 0.61. Thickness ranges from 350 to 4000 A. DRX measurements show an hcp structure. AGFM measurement gives saturation magnetization ranging from a negligible value to 120 emu/cm³. Coercive field may reach values up to 200 Oe, depending on the percentage of chromium. The saturation magnetization decreases as the Cr content increases. Magnetic force microscopy (MFM) study reveals the absence of stripe domains equilibrium magnetization structure. Brillouin light scattering (BLS) measurements were possible only for the 1800 A thick sample. They confirm, through the derived magnetic parameters, the absence of stripe magnetic domains as observed by MFM on one hand, and, on the other hand, the adjustment of theoretical and experimental results lead to a stiffness constant 10 times lower than pure Co one. These results are analyzed and correlated.

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A02	`01`			`@0 JMMMDC`
A03		`1`		`@0 J. magn. magn. mater.`
A05				`@2 310`
A06				`@2 1`
A08	`01`	`1`	`ENG`	`@1 Magnetic and structural properties of evaporated Co_xCr_1- _x/Si(1 00) and Co_xCr_1- _x/glass thin films`
A11	`01`	`1`		`@1 KHARMOUCHE (A.)`
A11	`02`	`1`		`@1 CHERIF (S.-M.)`
A11	`03`	`1`		`@1 SCHMERBER (G.)`
A11	`04`	`1`		`@1 BOURZAMI (A.)`
A14	`01`			`@1 Département de Physique, Université Ferhat Abbas @2 Sétif 19000 @3 DZA @Z 1 aut. @Z 4 aut.`
A14	`02`			`@1 Laboratoire PMTM, Institut Galilée, Université Paris 13 @2 Villetaneuse 93340 @3 FRA @Z 2 aut.`
A14	`03`			`@1 IPCMS-GEMME, UMR-CNRS, Université Louis Pasteur, 23 rue du Loess, B.P.43 @2 67034, Strasbourg @3 FRA @Z 3 aut.`
A20				`@1 152-158`
A21				`@1 2007`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 17230 @5 354000145235190210`
A44				`@0 0000 @1 © 2007 INIST-CNRS. All rights reserved.`
A45				`@0 26 ref.`
A47	`01`	`1`		`@0 07-0052715`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of magnetism and magnetic materials`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 Series of Co_xCr_1-x thin films have been evaporated under vacuum onto Si(1 0 0) and glass substrates, where x variations were between 0.51 and 0.61. Thickness ranges from 350 to 4000 A. DRX measurements show an hcp structure. AGFM measurement gives saturation magnetization ranging from a negligible value to 120 emu/cm³. Coercive field may reach values up to 200 Oe, depending on the percentage of chromium. The saturation magnetization decreases as the Cr content increases. Magnetic force microscopy (MFM) study reveals the absence of stripe domains equilibrium magnetization structure. Brillouin light scattering (BLS) measurements were possible only for the 1800 A thick sample. They confirm, through the derived magnetic parameters, the absence of stripe magnetic domains as observed by MFM on one hand, and, on the other hand, the adjustment of theoretical and experimental results lead to a stiffness constant 10 times lower than pure Co one. These results are analyzed and correlated.
C02	`01`	`3`		`@0 001B70E70C`
C02	`02`	`3`		`@0 001B70E70K`
C03	`01`	`3`	`FRE`	`@0 Propriété magnétique @5 02`
C03	`01`	`3`	`ENG`	`@0 Magnetic properties @5 02`
C03	`02`	`3`	`FRE`	`@0 Evaporation sous vide @5 03`
C03	`02`	`3`	`ENG`	`@0 Vacuum evaporation @5 03`
C03	`03`	`3`	`FRE`	`@0 Epaisseur @5 04`
C03	`03`	`3`	`ENG`	`@0 Thickness @5 04`
C03	`04`	`X`	`FRE`	`@0 Aimantation saturation @5 05`
C03	`04`	`X`	`ENG`	`@0 Saturation magnetization @5 05`
C03	`04`	`X`	`SPA`	`@0 Imanación saturación @5 05`
C03	`05`	`3`	`FRE`	`@0 Force coercitive @5 06`
C03	`05`	`3`	`ENG`	`@0 Coercive force @5 06`
C03	`06`	`3`	`FRE`	`@0 Microscopie force magnétique @5 07`
C03	`06`	`3`	`ENG`	`@0 Magnetic force microscopy @5 07`
C03	`07`	`3`	`FRE`	`@0 Structure domaine @5 08`
C03	`07`	`3`	`ENG`	`@0 Domain structure @5 08`
C03	`08`	`3`	`FRE`	`@0 Spectre Brillouin @5 09`
C03	`08`	`3`	`ENG`	`@0 Brillouin spectra @5 09`
C03	`09`	`3`	`FRE`	`@0 Hystérésis magnétique @5 10`
C03	`09`	`3`	`ENG`	`@0 Magnetic hysteresis @5 10`
C03	`10`	`3`	`FRE`	`@0 Domaine magnétique @5 11`
C03	`10`	`3`	`ENG`	`@0 Magnetic domains @5 11`
C03	`11`	`3`	`FRE`	`@0 Substrat @5 14`
C03	`11`	`3`	`ENG`	`@0 Substrates @5 14`
C03	`12`	`3`	`FRE`	`@0 Chrome alliage @5 15`
C03	`12`	`3`	`ENG`	`@0 Chromium alloys @5 15`
C03	`13`	`3`	`FRE`	`@0 Couche mince @5 16`
C03	`13`	`3`	`ENG`	`@0 Thin films @5 16`
C03	`14`	`3`	`FRE`	`@0 Réseau hexagonal compact @5 17`
C03	`14`	`3`	`ENG`	`@0 HCP lattices @5 17`
C03	`15`	`3`	`FRE`	`@0 Cobalt alliage @5 19`
C03	`15`	`3`	`ENG`	`@0 Cobalt alloys @5 19`
C03	`16`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C03	`16`	`3`	`ENG`	`@0 Transition element alloys @5 48`
C03	`17`	`3`	`FRE`	`@0 7570C @4 INC @5 60`
C03	`18`	`3`	`FRE`	`@0 7570K @4 INC @5 61`
C03	`19`	`3`	`FRE`	`@0 Domaine en rubans @4 CD @5 96`
C03	`19`	`3`	`ENG`	`@0 Stripe domains @4 CD @5 96`
N21				`@1 036`

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Le document en format XML

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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetic and structural properties of evaporated Co<sub>x</sub>
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 <sub>x</sub>
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<term>Domain structure</term>
<term>HCP lattices</term>
<term>Magnetic domains</term>
<term>Magnetic force microscopy</term>
<term>Magnetic hysteresis</term>
<term>Magnetic properties</term>
<term>Saturation magnetization</term>
<term>Stripe domains</term>
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<term>Transition element alloys</term>
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<term>Evaporation sous vide</term>
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<term>Force coercitive</term>
<term>Microscopie force magnétique</term>
<term>Structure domaine</term>
<term>Spectre Brillouin</term>
<term>Hystérésis magnétique</term>
<term>Domaine magnétique</term>
<term>Substrat</term>
<term>Chrome alliage</term>
<term>Couche mince</term>
<term>Réseau hexagonal compact</term>
<term>Cobalt alliage</term>
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<front><div type="abstract" xml:lang="en">Series of Co<sub>x</sub>
Cr<sub>1-x</sub>
 thin films have been evaporated under vacuum onto Si(1 0 0) and glass substrates, where x variations were between 0.51 and 0.61. Thickness ranges from 350 to 4000 A. DRX measurements show an hcp structure. AGFM measurement gives saturation magnetization ranging from a negligible value to 120 emu/cm<sup>3</sup>
. Coercive field may reach values up to 200 Oe, depending on the percentage of chromium. The saturation magnetization decreases as the Cr content increases. Magnetic force microscopy (MFM) study reveals the absence of stripe domains equilibrium magnetization structure. Brillouin light scattering (BLS) measurements were possible only for the 1800 A thick sample. They confirm, through the derived magnetic parameters, the absence of stripe magnetic domains as observed by MFM on one hand, and, on the other hand, the adjustment of theoretical and experimental results lead to a stiffness constant 10 times lower than pure Co one. These results are analyzed and correlated.</div>
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 <sub>x</sub>
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Cr<sub>1-</sub>
 <sub>x</sub>
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<fA14 i1="02"><s1>Laboratoire PMTM, Institut Galilée, Université Paris 13</s1>
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<fC01 i1="01" l="ENG"><s0>Series of Co<sub>x</sub>
Cr<sub>1-x</sub>
 thin films have been evaporated under vacuum onto Si(1 0 0) and glass substrates, where x variations were between 0.51 and 0.61. Thickness ranges from 350 to 4000 A. DRX measurements show an hcp structure. AGFM measurement gives saturation magnetization ranging from a negligible value to 120 emu/cm<sup>3</sup>
. Coercive field may reach values up to 200 Oe, depending on the percentage of chromium. The saturation magnetization decreases as the Cr content increases. Magnetic force microscopy (MFM) study reveals the absence of stripe domains equilibrium magnetization structure. Brillouin light scattering (BLS) measurements were possible only for the 1800 A thick sample. They confirm, through the derived magnetic parameters, the absence of stripe magnetic domains as observed by MFM on one hand, and, on the other hand, the adjustment of theoretical and experimental results lead to a stiffness constant 10 times lower than pure Co one. These results are analyzed and correlated.</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Propriété magnétique</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Magnetic properties</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Evaporation sous vide</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Vacuum evaporation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Epaisseur</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Thickness</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Aimantation saturation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Saturation magnetization</s0>
<s5>05</s5>
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<fC03 i1="04" i2="X" l="SPA"><s0>Imanación saturación</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Force coercitive</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Coercive force</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Microscopie force magnétique</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Magnetic force microscopy</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Structure domaine</s0>
<s5>08</s5>
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<fC03 i1="07" i2="3" l="ENG"><s0>Domain structure</s0>
<s5>08</s5>
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<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Brillouin spectra</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Hystérésis magnétique</s0>
<s5>10</s5>
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<fC03 i1="09" i2="3" l="ENG"><s0>Magnetic hysteresis</s0>
<s5>10</s5>
</fC03>
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<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Magnetic domains</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Substrat</s0>
<s5>14</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Substrates</s0>
<s5>14</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Chrome alliage</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Chromium alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Couche mince</s0>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Thin films</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Réseau hexagonal compact</s0>
<s5>17</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>HCP lattices</s0>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Cobalt alliage</s0>
<s5>19</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Cobalt alloys</s0>
<s5>19</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>48</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>48</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>7570C</s0>
<s4>INC</s4>
<s5>60</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>7570K</s0>
<s4>INC</s4>
<s5>61</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Domaine en rubans</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG"><s0>Stripe domains</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>036</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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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 structural properties of evaporated CoxCr1- x/Si(1 00) and CoxCr1- x/glass thin films

Magnetic and structural properties of evaporated CoxCr1- x/Si(1 00) and CoxCr1- x/glass thin films

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