CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000241

Critical behavior in Co-doped manganites La0.67Pb0.33Mn1-xCoxO3 (0 ≤ x ≤ 0.08)

Identifieur interne : 000241 ( PascalFrancis/Curation ); précédent : 000240; suivant : 000242

Critical behavior in Co-doped manganites La0.67Pb0.33Mn1-xCoxO3 (0 ≤ x ≤ 0.08)

Auteurs : N. Dhahri [Tunisie] ; J. Dhahri [Tunisie] ; E. K. Hlil [France] ; E. Dhahri [Tunisie]

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2012.

RBID : Pascal:12-0239500

Descripteurs français

Pascal (Inist)
- Phénomène critique, Dopage, Transition ferromagnétique paramagnétique, Exposant critique, Modèle Heisenberg, Approximation champ moyen, Concentration impureté, Ordre longue distance, Point critique, Loi échelle, Addition cobalt, Aimantation, Manganite, Perovskites, Diagramme d'Arrott.
Wicri :
- topic : Dopage.

English descriptors

KwdEn :
- Arrott plot, Cobalt additions, Critical exponents, Critical phenomena, Critical points, Doping, Ferromagnetic-paramagnetic transitions, Heisenberg model, Impurity density, Long-range order, Magnetization, Manganites, Mean field approximation, Perovskites, Scaling laws.

Abstract

The critical properties of perovskite manganite La_0.67Pb_0.33Mn_1-xCO_xO₃ (0 ≤ x ≤ 0.08) around the paramagnetic-ferromagnetic phase transition are investigated through various techniques such as the modified Arrott plot, Kouvel-Fisher method and critical isotherm analysis. Though the nature of this transition was found to be in second order, the estimated critical exponents β (0.233 ≤ β ≤ 0.368), γ (1.03 ≤γ≤ 1.40) and δ (4.32 < δ ≤ 5.54) are in between the theoretically predicted values for three-dimensional Heisenberg and tricritical mean-field model. This model suggests the coexistence of the short-range and long-range ferromagnetic orders around the critical temperature. The values of the critical exponents obtained from different methods and the well-obeyed scaling behavior confirm that the calculated exponents are unambiguous and purely intrinsic to the system.

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A03		`1`		`@0 J. magn. magn. mater.`
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A08	`01`	`1`	`ENG`	`@1 Critical behavior in Co-doped manganites La_0.67Pb_0.33Mn_1-xCo_xO₃ (0 ≤ x ≤ 0.08)`
A11	`01`	`1`		`@1 DHAHRI (N.)`
A11	`02`	`1`		`@1 DHAHRI (J.)`
A11	`03`	`1`		`@1 HLIL (E. K.)`
A11	`04`	`1`		`@1 DHAHRI (E.)`
A14	`01`			`@1 Unité de Recherche de Physique des Solides, Département de Physique, Faculté des Sciences de Monastir @2 5019 @3 TUN @Z 1 aut. @Z 2 aut.`
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A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 61 ref.`
A47	`01`	`1`		`@0 12-0239500`
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 critical properties of perovskite manganite La_0.67Pb_0.33Mn_1-xCO_xO₃ (0 ≤ x ≤ 0.08) around the paramagnetic-ferromagnetic phase transition are investigated through various techniques such as the modified Arrott plot, Kouvel-Fisher method and critical isotherm analysis. Though the nature of this transition was found to be in second order, the estimated critical exponents β (0.233 ≤ β ≤ 0.368), γ (1.03 ≤γ≤ 1.40) and δ (4.32 < δ ≤ 5.54) are in between the theoretically predicted values for three-dimensional Heisenberg and tricritical mean-field model. This model suggests the coexistence of the short-range and long-range ferromagnetic orders around the critical temperature. The values of the critical exponents obtained from different methods and the well-obeyed scaling behavior confirm that the calculated exponents are unambiguous and purely intrinsic to the system.
C02	`01`	`3`		`@0 001B70E47L`
C02	`02`	`3`		`@0 001B70E40C`
C03	`01`	`3`	`FRE`	`@0 Phénomène critique @5 02`
C03	`01`	`3`	`ENG`	`@0 Critical phenomena @5 02`
C03	`02`	`X`	`FRE`	`@0 Dopage @5 03`
C03	`02`	`X`	`ENG`	`@0 Doping @5 03`
C03	`02`	`X`	`SPA`	`@0 Doping @5 03`
C03	`03`	`3`	`FRE`	`@0 Transition ferromagnétique paramagnétique @5 04`
C03	`03`	`3`	`ENG`	`@0 Ferromagnetic-paramagnetic transitions @5 04`
C03	`04`	`3`	`FRE`	`@0 Exposant critique @5 05`
C03	`04`	`3`	`ENG`	`@0 Critical exponents @5 05`
C03	`05`	`3`	`FRE`	`@0 Modèle Heisenberg @5 06`
C03	`05`	`3`	`ENG`	`@0 Heisenberg model @5 06`
C03	`06`	`X`	`FRE`	`@0 Approximation champ moyen @5 07`
C03	`06`	`X`	`ENG`	`@0 Mean field approximation @5 07`
C03	`06`	`X`	`SPA`	`@0 Aproximación campo medio @5 07`
C03	`07`	`X`	`FRE`	`@0 Concentration impureté @5 08`
C03	`07`	`X`	`ENG`	`@0 Impurity density @5 08`
C03	`07`	`X`	`SPA`	`@0 Concentración impureza @5 08`
C03	`08`	`3`	`FRE`	`@0 Ordre longue distance @5 09`
C03	`08`	`3`	`ENG`	`@0 Long-range order @5 09`
C03	`09`	`3`	`FRE`	`@0 Point critique @5 10`
C03	`09`	`3`	`ENG`	`@0 Critical points @5 10`
C03	`10`	`3`	`FRE`	`@0 Loi échelle @5 11`
C03	`10`	`3`	`ENG`	`@0 Scaling laws @5 11`
C03	`11`	`3`	`FRE`	`@0 Addition cobalt @5 12`
C03	`11`	`3`	`ENG`	`@0 Cobalt additions @5 12`
C03	`12`	`3`	`FRE`	`@0 Aimantation @5 13`
C03	`12`	`3`	`ENG`	`@0 Magnetization @5 13`
C03	`13`	`X`	`FRE`	`@0 Manganite @2 NA @5 15`
C03	`13`	`X`	`ENG`	`@0 Manganites @2 NA @5 15`
C03	`13`	`X`	`SPA`	`@0 Manganito @2 NA @5 15`
C03	`14`	`3`	`FRE`	`@0 Perovskites @5 16`
C03	`14`	`3`	`ENG`	`@0 Perovskites @5 16`
C03	`15`	`3`	`FRE`	`@0 Diagramme d'Arrott @4 CD @5 96`
C03	`15`	`3`	`ENG`	`@0 Arrott plot @4 CD @5 96`
N21				`@1 184`

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Le document en format XML

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<term>Modèle Heisenberg</term>
<term>Approximation champ moyen</term>
<term>Concentration impureté</term>
<term>Ordre longue distance</term>
<term>Point critique</term>
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<term>Addition cobalt</term>
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<front><div type="abstract" xml:lang="en">The critical properties of perovskite manganite La<sub>0.67</sub>
Pb<sub>0.33</sub>
Mn<sub>1-x</sub>
CO<sub>x</sub>
O<sub>3</sub>
 (0 ≤ x ≤ 0.08) around the paramagnetic-ferromagnetic phase transition are investigated through various techniques such as the modified Arrott plot, Kouvel-Fisher method and critical isotherm analysis. Though the nature of this transition was found to be in second order, the estimated critical exponents β (0.233 ≤ β ≤ 0.368), γ (1.03 ≤γ≤ 1.40) and δ (4.32 < δ ≤ 5.54) are in between the theoretically predicted values for three-dimensional Heisenberg and tricritical mean-field model. This model suggests the coexistence of the short-range and long-range ferromagnetic orders around the critical temperature. The values of the critical exponents obtained from different methods and the well-obeyed scaling behavior confirm that the calculated exponents are unambiguous and purely intrinsic to the system.</div>
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Pb<sub>0.33</sub>
Mn<sub>1-x</sub>
Co<sub>x</sub>
O<sub>3 </sub>
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<fC01 i1="01" l="ENG"><s0>The critical properties of perovskite manganite La<sub>0.67</sub>
Pb<sub>0.33</sub>
Mn<sub>1-x</sub>
CO<sub>x</sub>
O<sub>3</sub>
 (0 ≤ x ≤ 0.08) around the paramagnetic-ferromagnetic phase transition are investigated through various techniques such as the modified Arrott plot, Kouvel-Fisher method and critical isotherm analysis. Though the nature of this transition was found to be in second order, the estimated critical exponents β (0.233 ≤ β ≤ 0.368), γ (1.03 ≤γ≤ 1.40) and δ (4.32 < δ ≤ 5.54) are in between the theoretically predicted values for three-dimensional Heisenberg and tricritical mean-field model. This model suggests the coexistence of the short-range and long-range ferromagnetic orders around the critical temperature. The values of the critical exponents obtained from different methods and the well-obeyed scaling behavior confirm that the calculated exponents are unambiguous and purely intrinsic to the system.</s0>
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<s5>03</s5>
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<s5>03</s5>
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<fC03 i1="02" i2="X" l="SPA"><s0>Doping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Transition ferromagnétique paramagnétique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Ferromagnetic-paramagnetic transitions</s0>
<s5>04</s5>
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<fC03 i1="04" i2="3" l="FRE"><s0>Exposant critique</s0>
<s5>05</s5>
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<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Modèle Heisenberg</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Heisenberg model</s0>
<s5>06</s5>
</fC03>
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<s5>07</s5>
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<s5>07</s5>
</fC03>
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<s5>07</s5>
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<s5>08</s5>
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<s5>08</s5>
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<s5>08</s5>
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<s5>09</s5>
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<s5>09</s5>
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<s5>10</s5>
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<fC03 i1="09" i2="3" l="ENG"><s0>Critical points</s0>
<s5>10</s5>
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<fC03 i1="10" i2="3" l="FRE"><s0>Loi échelle</s0>
<s5>11</s5>
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<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Addition cobalt</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Cobalt additions</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Aimantation</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Magnetization</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Manganite</s0>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Manganites</s0>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Manganito</s0>
<s2>NA</s2>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Perovskites</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Perovskites</s0>
<s5>16</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Diagramme d'Arrott</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Arrott plot</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>184</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Critical behavior in Co-doped manganites La0.67Pb0.33Mn1-xCoxO3 (0 ≤ x ≤ 0.08)

Critical behavior in Co-doped manganites La0.67Pb0.33Mn1-xCoxO3 (0 ≤ x ≤ 0.08)

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