CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000282

Effect of the applied magnetic field and the layer thickness on the magnon properties in bilayers Co/Pt and symmetrical trilayer Pt/Co/Pt

Identifieur interne : 000282 ( PascalFrancis/Curation ); précédent : 000281; suivant : 000283

Effect of the applied magnetic field and the layer thickness on the magnon properties in bilayers Co/Pt and symmetrical trilayer Pt/Co/Pt

Auteurs : M. Mehdioui [Maroc] ; A. Fahmi [Maroc] ; H. Lassri [Maroc] ; M. Fahoume [Maroc] ; A. Qachaou [Maroc]

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2014.

RBID : Pascal:14-0108075

Descripteurs français

Pascal (Inist)
- Effet champ magnétique, Magnon, Magnon surface, Onde spin, Modèle Heisenberg, Hamiltonien spin, Anisotropie, Interaction échange, Interaction dipolaire, Spectre excitation, Sous bande, Bicouche, Multicouche, Platine, Cobalt, Métal transition.
Wicri :
- topic : Platine, Cobalt.

English descriptors

KwdEn :
- Anisotropy, Bilayers, Cobalt, Dipole interactions, Exchange interactions, Excitation spectrum, Heisenberg model, Magnetic field effects, Magnons, Multilayers, Platinum, Spin Hamiltonians, Spin waves, Subband, Surface magnons, Transition elements.

Abstract

We have studied the elementary magnetic excitations and their dynamics in multilayer Co(t Co)/Pt(t Pt) and Pt(f Pt)/Co(t Co)/Pt(t Pt) under an applied magnetic field. The Heisenberg hamiltonian used takes into account the magneto-crystalline and surface anisotropies, the exchange and dipolar interactions. The calculated excitation spectrum ε_N(k) presents a structure with two sub-bands corresponding to the magnons of surface and volume respectively. The existence of a gap of creating these magnons is also highlighted. The lifetimes deduced from these gaps are in good agreement with the results of previous studies. The thermal evolution of the magnetization m_z indicates that the system undergoes a dimensional crossover 3D-2D when the temperature increases. The calculated and measured magnetizations are compared and they are in good agreement. The exchange integral and critical temperature values deduced from these adjustments are in very good agreement with the results of previous works.

A01	`01`	`1`		`@0 0304-8853`
A02	`01`			`@0 JMMMDC`
A03		`1`		`@0 J. magn. magn. mater.`
A05				`@2 352`
A08	`01`	`1`	`ENG`	`@1 Effect of the applied magnetic field and the layer thickness on the magnon properties in bilayers Co/Pt and symmetrical trilayer Pt/Co/Pt`
A11	`01`	`1`		`@1 MEHDIOUI (M.)`
A11	`02`	`1`		`@1 FAHMI (A.)`
A11	`03`	`1`		`@1 LASSRI (H.)`
A11	`04`	`1`		`@1 FAHOUME (M.)`
A11	`05`	`1`		`@1 QACHAOU (A.)`
A14	`01`			`@1 Laboratoire de physique de la matière condensée (LPMC), Faculté des Sciences, B.P. 133-14000 @2 Kenitra @3 MAR @Z 1 aut. @Z 2 aut. @Z 4 aut. @Z 5 aut.`
A14	`02`			`@1 Laboratoire de physique des matériaux (LPM), Faculté des Sciences, Ain chock Mâarif B.P. 5366 @2 Casablanca @3 MAR @Z 3 aut.`
A20				`@1 107-114`
A21				`@1 2014`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 17230 @5 354000506170350170`
A44				`@0 0000 @1 © 2014 INIST-CNRS. All rights reserved.`
A45				`@0 19 ref.`
A47	`01`	`1`		`@0 14-0108075`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of magnetism and magnetic materials`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 We have studied the elementary magnetic excitations and their dynamics in multilayer Co(t Co)/Pt(t Pt) and Pt(f Pt)/Co(t Co)/Pt(t Pt) under an applied magnetic field. The Heisenberg hamiltonian used takes into account the magneto-crystalline and surface anisotropies, the exchange and dipolar interactions. The calculated excitation spectrum ε_N(k) presents a structure with two sub-bands corresponding to the magnons of surface and volume respectively. The existence of a gap of creating these magnons is also highlighted. The lifetimes deduced from these gaps are in good agreement with the results of previous studies. The thermal evolution of the magnetization m_z indicates that the system undergoes a dimensional crossover 3D-2D when the temperature increases. The calculated and measured magnetizations are compared and they are in good agreement. The exchange integral and critical temperature values deduced from these adjustments are in very good agreement with the results of previous works.
C02	`01`	`3`		`@0 001B70E30D`
C02	`02`	`3`		`@0 001B70E70C`
C03	`01`	`3`	`FRE`	`@0 Effet champ magnétique @5 02`
C03	`01`	`3`	`ENG`	`@0 Magnetic field effects @5 02`
C03	`02`	`3`	`FRE`	`@0 Magnon @5 03`
C03	`02`	`3`	`ENG`	`@0 Magnons @5 03`
C03	`03`	`3`	`FRE`	`@0 Magnon surface @5 05`
C03	`03`	`3`	`ENG`	`@0 Surface magnons @5 05`
C03	`04`	`3`	`FRE`	`@0 Onde spin @5 06`
C03	`04`	`3`	`ENG`	`@0 Spin waves @5 06`
C03	`05`	`3`	`FRE`	`@0 Modèle Heisenberg @5 07`
C03	`05`	`3`	`ENG`	`@0 Heisenberg model @5 07`
C03	`06`	`3`	`FRE`	`@0 Hamiltonien spin @5 08`
C03	`06`	`3`	`ENG`	`@0 Spin Hamiltonians @5 08`
C03	`07`	`3`	`FRE`	`@0 Anisotropie @5 09`
C03	`07`	`3`	`ENG`	`@0 Anisotropy @5 09`
C03	`08`	`3`	`FRE`	`@0 Interaction échange @5 10`
C03	`08`	`3`	`ENG`	`@0 Exchange interactions @5 10`
C03	`09`	`3`	`FRE`	`@0 Interaction dipolaire @5 11`
C03	`09`	`3`	`ENG`	`@0 Dipole interactions @5 11`
C03	`10`	`X`	`FRE`	`@0 Spectre excitation @5 12`
C03	`10`	`X`	`ENG`	`@0 Excitation spectrum @5 12`
C03	`10`	`X`	`SPA`	`@0 Espectro excitación @5 12`
C03	`11`	`X`	`FRE`	`@0 Sous bande @5 13`
C03	`11`	`X`	`ENG`	`@0 Subband @5 13`
C03	`11`	`X`	`SPA`	`@0 Subbanda @5 13`
C03	`12`	`3`	`FRE`	`@0 Bicouche @5 15`
C03	`12`	`3`	`ENG`	`@0 Bilayers @5 15`
C03	`13`	`3`	`FRE`	`@0 Multicouche @5 16`
C03	`13`	`3`	`ENG`	`@0 Multilayers @5 16`
C03	`14`	`3`	`FRE`	`@0 Platine @2 NC @5 17`
C03	`14`	`3`	`ENG`	`@0 Platinum @2 NC @5 17`
C03	`15`	`3`	`FRE`	`@0 Cobalt @2 NC @5 18`
C03	`15`	`3`	`ENG`	`@0 Cobalt @2 NC @5 18`
C03	`16`	`3`	`FRE`	`@0 Métal transition @5 48`
C03	`16`	`3`	`ENG`	`@0 Transition elements @5 48`
N21				`@1 146`

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Le document en format XML

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<term>Exchange interactions</term>
<term>Excitation spectrum</term>
<term>Heisenberg model</term>
<term>Magnetic field effects</term>
<term>Magnons</term>
<term>Multilayers</term>
<term>Platinum</term>
<term>Spin Hamiltonians</term>
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<term>Transition elements</term>
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<term>Onde spin</term>
<term>Modèle Heisenberg</term>
<term>Hamiltonien spin</term>
<term>Anisotropie</term>
<term>Interaction échange</term>
<term>Interaction dipolaire</term>
<term>Spectre excitation</term>
<term>Sous bande</term>
<term>Bicouche</term>
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<term>Platine</term>
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<front><div type="abstract" xml:lang="en">We have studied the elementary magnetic excitations and their dynamics in multilayer Co(t Co)/Pt(t Pt) and Pt(f Pt)/Co(t Co)/Pt(t Pt) under an applied magnetic field. The Heisenberg hamiltonian used takes into account the magneto-crystalline and surface anisotropies, the exchange and dipolar interactions. The calculated excitation spectrum ε<sub>N</sub>
(k) presents a structure with two sub-bands corresponding to the magnons of surface and volume respectively. The existence of a gap of creating these magnons is also highlighted. The lifetimes deduced from these gaps are in good agreement with the results of previous studies. The thermal evolution of the magnetization m<sub>z</sub>
 indicates that the system undergoes a dimensional crossover 3D-2D when the temperature increases. The calculated and measured magnetizations are compared and they are in good agreement. The exchange integral and critical temperature values deduced from these adjustments are in very good agreement with the results of previous works.</div>
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<fA11 i1="01" i2="1"><s1>MEHDIOUI (M.)</s1>
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<fA14 i1="01"><s1>Laboratoire de physique de la matière condensée (LPMC), Faculté des Sciences, B.P. 133-14000</s1>
<s2>Kenitra</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Laboratoire de physique des matériaux (LPM), Faculté des Sciences, Ain chock Mâarif B.P. 5366</s1>
<s2>Casablanca</s2>
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<sZ>3 aut.</sZ>
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<fA60><s1>P</s1>
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<fC01 i1="01" l="ENG"><s0>We have studied the elementary magnetic excitations and their dynamics in multilayer Co(t Co)/Pt(t Pt) and Pt(f Pt)/Co(t Co)/Pt(t Pt) under an applied magnetic field. The Heisenberg hamiltonian used takes into account the magneto-crystalline and surface anisotropies, the exchange and dipolar interactions. The calculated excitation spectrum ε<sub>N</sub>
(k) presents a structure with two sub-bands corresponding to the magnons of surface and volume respectively. The existence of a gap of creating these magnons is also highlighted. The lifetimes deduced from these gaps are in good agreement with the results of previous studies. The thermal evolution of the magnetization m<sub>z</sub>
 indicates that the system undergoes a dimensional crossover 3D-2D when the temperature increases. The calculated and measured magnetizations are compared and they are in good agreement. The exchange integral and critical temperature values deduced from these adjustments are in very good agreement with the results of previous works.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E30D</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Effet champ magnétique</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Magnetic field effects</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Magnon</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Magnons</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Magnon surface</s0>
<s5>05</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Surface magnons</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Onde spin</s0>
<s5>06</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Spin waves</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Modèle Heisenberg</s0>
<s5>07</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Heisenberg model</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Hamiltonien spin</s0>
<s5>08</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Spin Hamiltonians</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Anisotropie</s0>
<s5>09</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Anisotropy</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Interaction échange</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Exchange interactions</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Interaction dipolaire</s0>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Dipole interactions</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Spectre excitation</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Excitation spectrum</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Espectro excitación</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Sous bande</s0>
<s5>13</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Subband</s0>
<s5>13</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Subbanda</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Bicouche</s0>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Bilayers</s0>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Multicouche</s0>
<s5>16</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Multilayers</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Platine</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Platinum</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>18</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Cobalt</s0>
<s2>NC</s2>
<s5>18</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Métal transition</s0>
<s5>48</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Transition elements</s0>
<s5>48</s5>
</fC03>
<fN21><s1>146</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

Effect of the applied magnetic field and the layer thickness on the magnon properties in bilayers Co/Pt and symmetrical trilayer Pt/Co/Pt

Effect of the applied magnetic field and the layer thickness on the magnon properties in bilayers Co/Pt and symmetrical trilayer Pt/Co/Pt

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