NickelMaghrebV1, PascalFrancis, Curation, bibRecord, 000417

Magnetic properties of mixed Ni-Cu ferrites calculated using mean field approach

Identifieur interne : 000417 ( PascalFrancis/Curation ); précédent : 000416; suivant : 000418

Magnetic properties of mixed Ni-Cu ferrites calculated using mean field approach

Auteurs : R. Masrour [Maroc] ; M. Hamedoun [Maroc] ; A. Benyoussef [Maroc] ; E. K. Hlil [France]

Source :

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

RBID : Pascal:14-0154334

Descripteurs français

Pascal (Inist)
- Approximation champ moyen, Développement série, Approximation Padé, Point critique, Aimantation saturation, Sous réseau, Interaction échange, Loi probabilité, Exposant critique, Susceptibilité magnétique, Ferrites spinelles, Fer Nickel Oxyde Mixte.

English descriptors

KwdEn :
- Critical exponents, Critical points, Exchange interactions, Ferrites spinels, Iron Nickel Oxides Mixed, Magnetic susceptibility, Mean field approximation, Padé approximation, Probability distribution, Saturation magnetization, Series expansion, Sublattices.

Abstract

The magnetic properties of spinel ferrites [Fe³⁺_1-(1-x)yCu²⁺_(1-x)y]_A[Ni²⁺_xCu²⁺_(1-x)(1-y)Fe³⁺_1+(1-x)y]_BO₄ have been studied by the mean field theory (MFT) and high temperature series expansions (HTSEs) combined with the Padé approximants. The critical temperature, the saturation magnetisation (M_s) and the intra-sublattice exchanges interactions (J_AA(x,y), J_BB(x,y) and J_AB(x,y)) are obtained by using a probability distribution law. The critical exponents associate with the magnetic susceptibility have been obtained. The effect of copper doping on the magnetic properties of nickel ferrites has been examined.

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A03		`1`		`@0 J. magn. magn. mater.`
A05				`@2 363`
A08	`01`	`1`	`ENG`	`@1 Magnetic properties of mixed Ni-Cu ferrites calculated using mean field approach`
A11	`01`	`1`		`@1 MASROUR (R.)`
A11	`02`	`1`		`@1 HAMEDOUN (M.)`
A11	`03`	`1`		`@1 BENYOUSSEF (A.)`
A11	`04`	`1`		`@1 HLIL (E. K.)`
A14	`01`			`@1 Laboratory of Materials, Processes, Environment and Quality, Cady Ayyed University, National School of Applied Sciences, 63 @2 46000 Safi @3 MAR @Z 1 aut.`
A14	`02`			`@1 LMPHE, URAC 12, Faculté des Sciences, Université Mohamed V-Agdal @2 Rabat @3 MAR @Z 1 aut. @Z 3 aut.`
A14	`03`			`@1 Institute for Nanomaterials and Nanotechnologies, MAScIR @2 Rabat @3 MAR @Z 2 aut. @Z 3 aut.`
A14	`04`			`@1 Academie Hassan II des Sciences et Techniques @2 Rabat @3 MAR @Z 3 aut.`
A14	`05`			`@1 Institut Néel, CNRS et Université Joseph Fourier, BP 166 @2 38042 Grenoble @3 FRA @Z 4 aut.`
A20				`@1 1-5`
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A44				`@0 0000 @1 © 2014 INIST-CNRS. All rights reserved.`
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A61				`@0 A`
A64	`01`	`1`		`@0 Journal of magnetism and magnetic materials`
A66	`01`			`@0 NLD`
C01	`01`		`ENG`	@0 The magnetic properties of spinel ferrites [Fe³⁺_1-(1-x)yCu²⁺_(1-x)y]_A[Ni²⁺_xCu²⁺_(1-x)(1-y)Fe³⁺_1+(1-x)y]_BO₄ have been studied by the mean field theory (MFT) and high temperature series expansions (HTSEs) combined with the Padé approximants. The critical temperature, the saturation magnetisation (M_s) and the intra-sublattice exchanges interactions (J_AA(x,y), J_BB(x,y) and J_AB(x,y)) are obtained by using a probability distribution law. The critical exponents associate with the magnetic susceptibility have been obtained. The effect of copper doping on the magnetic properties of nickel ferrites has been examined.
C02	`01`	`3`		`@0 001B70E40C`
C03	`01`	`X`	`FRE`	`@0 Approximation champ moyen @5 03`
C03	`01`	`X`	`ENG`	`@0 Mean field approximation @5 03`
C03	`01`	`X`	`SPA`	`@0 Aproximación campo medio @5 03`
C03	`02`	`3`	`FRE`	`@0 Développement série @5 05`
C03	`02`	`3`	`ENG`	`@0 Series expansion @5 05`
C03	`03`	`3`	`FRE`	`@0 Approximation Padé @5 06`
C03	`03`	`3`	`ENG`	`@0 Padé approximation @5 06`
C03	`04`	`3`	`FRE`	`@0 Point critique @5 07`
C03	`04`	`3`	`ENG`	`@0 Critical points @5 07`
C03	`05`	`X`	`FRE`	`@0 Aimantation saturation @5 08`
C03	`05`	`X`	`ENG`	`@0 Saturation magnetization @5 08`
C03	`05`	`X`	`SPA`	`@0 Imanación saturación @5 08`
C03	`06`	`3`	`FRE`	`@0 Sous réseau @5 09`
C03	`06`	`3`	`ENG`	`@0 Sublattices @5 09`
C03	`07`	`3`	`FRE`	`@0 Interaction échange @5 10`
C03	`07`	`3`	`ENG`	`@0 Exchange interactions @5 10`
C03	`08`	`X`	`FRE`	`@0 Loi probabilité @5 11`
C03	`08`	`X`	`ENG`	`@0 Probability distribution @5 11`
C03	`08`	`X`	`SPA`	`@0 Ley probabilidad @5 11`
C03	`09`	`3`	`FRE`	`@0 Exposant critique @5 12`
C03	`09`	`3`	`ENG`	`@0 Critical exponents @5 12`
C03	`10`	`3`	`FRE`	`@0 Susceptibilité magnétique @5 13`
C03	`10`	`3`	`ENG`	`@0 Magnetic susceptibility @5 13`
C03	`11`	`X`	`FRE`	`@0 Ferrites spinelles @5 17`
C03	`11`	`X`	`ENG`	`@0 Ferrites spinels @5 17`
C03	`11`	`X`	`SPA`	`@0 Feritas espinelas @5 17`
C03	`12`	`X`	`FRE`	`@0 Fer Nickel Oxyde Mixte @2 NC @2 NA @5 18`
C03	`12`	`X`	`ENG`	`@0 Iron Nickel Oxides Mixed @2 NC @2 NA @5 18`
C03	`12`	`X`	`SPA`	`@0 Mixto @2 NC @2 NA @5 18`
N21				`@1 195`

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Le document en format XML

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<author><name sortKey="Hamedoun, M" sort="Hamedoun, M" uniqKey="Hamedoun M" first="M." last="Hamedoun">M. Hamedoun</name>
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<term>Iron Nickel Oxides Mixed</term>
<term>Magnetic susceptibility</term>
<term>Mean field approximation</term>
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<front><div type="abstract" xml:lang="en">The magnetic properties of spinel ferrites [Fe<sup>3+</sup>
<sub>1-(1-x)y</sub>
Cu<sup>2+</sup>
<sub>(1-x)y</sub>
]<sub>A</sub>
[Ni<sup>2+</sup>
<sub>x</sub>
Cu<sup>2+</sup>
<sub>(1-x)(1-y</sub>
)Fe<sup>3+</sup>
<sub>1+(1-x)y</sub>
]<sub>B</sub>
O<sub>4</sub>
 have been studied by the mean field theory (MFT) and high temperature series expansions (HTSEs) combined with the Padé approximants. The critical temperature, the saturation magnetisation (M<sub>s</sub>
) and the intra-sublattice exchanges interactions (J<sub>AA</sub>
(x,y), J<sub>BB</sub>
(x,y) and J<sub>AB</sub>
(x,y)) are obtained by using a probability distribution law. The critical exponents associate with the magnetic susceptibility have been obtained. The effect of copper doping on the magnetic properties of nickel ferrites has been examined.</div>
</front>
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<sZ>1 aut.</sZ>
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<fA14 i1="02"><s1>LMPHE, URAC 12, Faculté des Sciences, Université Mohamed V-Agdal</s1>
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<sZ>3 aut.</sZ>
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<sZ>3 aut.</sZ>
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<sZ>4 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>The magnetic properties of spinel ferrites [Fe<sup>3+</sup>
<sub>1-(1-x)y</sub>
Cu<sup>2+</sup>
<sub>(1-x)y</sub>
]<sub>A</sub>
[Ni<sup>2+</sup>
<sub>x</sub>
Cu<sup>2+</sup>
<sub>(1-x)(1-y</sub>
)Fe<sup>3+</sup>
<sub>1+(1-x)y</sub>
]<sub>B</sub>
O<sub>4</sub>
 have been studied by the mean field theory (MFT) and high temperature series expansions (HTSEs) combined with the Padé approximants. The critical temperature, the saturation magnetisation (M<sub>s</sub>
) and the intra-sublattice exchanges interactions (J<sub>AA</sub>
(x,y), J<sub>BB</sub>
(x,y) and J<sub>AB</sub>
(x,y)) are obtained by using a probability distribution law. The critical exponents associate with the magnetic susceptibility have been obtained. The effect of copper doping on the magnetic properties of nickel ferrites has been examined.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E40C</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Approximation champ moyen</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Mean field approximation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Aproximación campo medio</s0>
<s5>03</s5>
</fC03>
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<s5>05</s5>
</fC03>
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<s5>05</s5>
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<s5>06</s5>
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<s5>07</s5>
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<s5>07</s5>
</fC03>
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<s5>08</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Saturation magnetization</s0>
<s5>08</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Imanación saturación</s0>
<s5>08</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Sous réseau</s0>
<s5>09</s5>
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<s5>09</s5>
</fC03>
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<s5>10</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Exchange interactions</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Loi probabilité</s0>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Probability distribution</s0>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Ley probabilidad</s0>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Exposant critique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Critical exponents</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Susceptibilité magnétique</s0>
<s5>13</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Magnetic susceptibility</s0>
<s5>13</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Ferrites spinelles</s0>
<s5>17</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Ferrites spinels</s0>
<s5>17</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Feritas espinelas</s0>
<s5>17</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Fer Nickel Oxyde Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Iron Nickel Oxides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Mixto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>18</s5>
</fC03>
<fN21><s1>195</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Magnetic properties of mixed Ni-Cu ferrites calculated using mean field approach

Magnetic properties of mixed Ni-Cu ferrites calculated using mean field approach

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