ThuliumV1, Pascal, Corpus, bibRecord, 001351

Magnetic and electrical resistivity study of Tm3Co11B4 compound

Identifieur interne : 001351 ( Pascal/Corpus ); précédent : 001350; suivant : 001352

Magnetic and electrical resistivity study of Tm3Co11B4 compound

Auteurs : A. Kowalczyk ; L. Smardz

Source :

Journal of alloys and compounds [ 0925-8388 ] ; 1997.

RBID : Pascal:97-0487890

Descripteurs français

Pascal (Inist)
- Aimantation, Force coercitive, Conductivité électrique, Hystérésis magnétique, Effet champ magnétique, Réseau hexagonal, Point compensation, Interaction électron électron, Diffusion, Onde spin, Alliage base cobalt, Thulium alliage, Bore alliage, Alliage ternaire, Etude expérimentale, 7560E, 7215E, Alliage Co54Tm42B4, B Co Tm.

English descriptors

KwdEn :
- Boron alloys, Cobalt base alloys, Coercive force, Compensation point, Electric conductivity, Electron-electron interactions, Experimental study, Hexagonal lattices, Magnetic field effects, Magnetic hysteresis, Magnetization, Scattering, Spin waves, Ternary alloys, Thulium alloys.

Abstract

Copyright (c) 1997 Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm₃Co₁₁B₄ compound have been studied. This compound crystallizes in the hexagonal Ce₃Co₁₁B₄ type structure. Results show that the Tm₃Co₁₁B₄ is a ferromagnet with T_C=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm₃Co₁₁B₄ compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T² dependence, implying that electron-spin wave scattering is dominant in this temperature range.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0925-8388`
A03		`1`		`@0 J. alloys compd.`
A05				`@2 259`
A08	`01`	`1`	`ENG`	`@1 Magnetic and electrical resistivity study of Tm₃Co₁₁B₄ compound`
A11	`01`	`1`		`@1 KOWALCZYK (A.)`
A11	`02`	`1`		`@1 SMARDZ (L.)`
A14	`01`			`@1 Institute of Molecular Physics, Polish Academy of Sciences, Smoluchowskiego 17, 60-179 @2 Poznań @3 POL @Z 1 aut. @Z 2 aut.`
A20				`@1 59-61`
A21				`@1 1997`
A23	`01`			`@0 ENG`
A24	`01`			`@0 eng`
A43	`01`			`@1 INIST @2 1151 @5 354000069167050026`
A44				`@0 9000 @1 © 1997 Elsevier Science B.V. All rights reserved.`
A47	`01`	`1`		`@0 97-0487890`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of alloys and compounds`
A66	`01`			`@0 CHE`
C01	`01`		`ENG`	@0 Copyright (c) 1997 Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm₃Co₁₁B₄ compound have been studied. This compound crystallizes in the hexagonal Ce₃Co₁₁B₄ type structure. Results show that the Tm₃Co₁₁B₄ is a ferromagnet with T_C=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm₃Co₁₁B₄ compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T² dependence, implying that electron-spin wave scattering is dominant in this temperature range.
C02	`01`	`3`		`@0 001B70E60E`
C02	`02`	`3`		`@0 001B70B15E`
C02	`03`	`X`		`@0 240`
C03	`01`	`3`	`FRE`	`@0 Aimantation @5 02`
C03	`01`	`3`	`ENG`	`@0 Magnetization @5 02`
C03	`02`	`3`	`FRE`	`@0 Force coercitive @5 03`
C03	`02`	`3`	`ENG`	`@0 Coercive force @5 03`
C03	`03`	`3`	`FRE`	`@0 Conductivité électrique @5 04`
C03	`03`	`3`	`ENG`	`@0 Electric conductivity @5 04`
C03	`04`	`X`	`FRE`	`@0 Hystérésis magnétique @5 05`
C03	`04`	`X`	`ENG`	`@0 Magnetic hysteresis @5 05`
C03	`04`	`X`	`GER`	`@0 Magnetische Hysteresis @5 05`
C03	`04`	`X`	`SPA`	`@0 Histérisis magnética @5 05`
C03	`05`	`3`	`FRE`	`@0 Effet champ magnétique @5 06`
C03	`05`	`3`	`ENG`	`@0 Magnetic field effects @5 06`
C03	`06`	`3`	`FRE`	`@0 Réseau hexagonal @5 07`
C03	`06`	`3`	`ENG`	`@0 Hexagonal lattices @5 07`
C03	`07`	`X`	`FRE`	`@0 Point compensation @5 08`
C03	`07`	`X`	`ENG`	`@0 Compensation point @5 08`
C03	`07`	`X`	`SPA`	`@0 Punto compensación @5 08`
C03	`08`	`3`	`FRE`	`@0 Interaction électron électron @5 09`
C03	`08`	`3`	`ENG`	`@0 Electron-electron interactions @5 09`
C03	`09`	`3`	`FRE`	`@0 Diffusion @5 10`
C03	`09`	`3`	`ENG`	`@0 Scattering @5 10`
C03	`10`	`3`	`FRE`	`@0 Onde spin @5 11`
C03	`10`	`3`	`ENG`	`@0 Spin waves @5 11`
C03	`11`	`3`	`FRE`	`@0 Alliage base cobalt @2 NK @5 12`
C03	`11`	`3`	`ENG`	`@0 Cobalt base alloys @2 NK @5 12`
C03	`12`	`3`	`FRE`	`@0 Thulium alliage @5 13`
C03	`12`	`3`	`ENG`	`@0 Thulium alloys @5 13`
C03	`13`	`3`	`FRE`	`@0 Bore alliage @5 14`
C03	`13`	`3`	`ENG`	`@0 Boron alloys @5 14`
C03	`14`	`3`	`FRE`	`@0 Alliage ternaire @5 15`
C03	`14`	`3`	`ENG`	`@0 Ternary alloys @5 15`
C03	`15`	`3`	`FRE`	`@0 Etude expérimentale @5 18`
C03	`15`	`3`	`ENG`	`@0 Experimental study @5 18`
C03	`16`	`3`	`FRE`	`@0 7560E @2 PAC @4 INC @5 56`
C03	`17`	`3`	`FRE`	`@0 7215E @2 PAC @4 INC @5 57`
C03	`18`	`3`	`FRE`	`@0 Alliage Co54Tm42B4 @2 NK @4 INC @5 92`
C03	`19`	`3`	`FRE`	`@0 B Co Tm @4 INC @5 93`
C07	`01`	`3`	`FRE`	`@0 Lanthanide alliage @5 16`
C07	`01`	`3`	`ENG`	`@0 Rare earth alloys @5 16`
C07	`02`	`3`	`FRE`	`@0 Métal transition alliage @5 17`
C07	`02`	`3`	`ENG`	`@0 Transition element alloys @5 17`
N21				`@1 300`

Format Inist (serveur)

NO :	PASCAL 97-0487890 Elsevier
ET :	Magnetic and electrical resistivity study of Tm₃Co₁₁B₄ compound
AU :	KOWALCZYK (A.); SMARDZ (L.)
AF :	Institute of Molecular Physics, Polish Academy of Sciences, Smoluchowskiego 17, 60-179/Poznań/Pologne (1 aut., 2 aut.)
DT :	Publication en série; Niveau analytique
SO :	Journal of alloys and compounds; ISSN 0925-8388; Suisse; Da. 1997; Vol. 259; Pp. 59-61; Abs. anglais
LA :	Anglais
EA :	Copyright (c) 1997 Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm₃Co₁₁B₄ compound have been studied. This compound crystallizes in the hexagonal Ce₃Co₁₁B₄ type structure. Results show that the Tm₃Co₁₁B₄ is a ferromagnet with T_C=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm₃Co₁₁B₄ compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T² dependence, implying that electron-spin wave scattering is dominant in this temperature range.
CC :	001B70E60E; 001B70B15E; 240
FD :	Aimantation; Force coercitive; Conductivité électrique; Hystérésis magnétique; Effet champ magnétique; Réseau hexagonal; Point compensation; Interaction électron électron; Diffusion; Onde spin; Alliage base cobalt; Thulium alliage; Bore alliage; Alliage ternaire; Etude expérimentale; 7560E; 7215E; Alliage Co54Tm42B4; B Co Tm
FG :	Lanthanide alliage; Métal transition alliage
ED :	Magnetization; Coercive force; Electric conductivity; Magnetic hysteresis; Magnetic field effects; Hexagonal lattices; Compensation point; Electron-electron interactions; Scattering; Spin waves; Cobalt base alloys; Thulium alloys; Boron alloys; Ternary alloys; Experimental study
EG :	Rare earth alloys; Transition element alloys
GD :	Magnetische Hysteresis
SD :	Histérisis magnética; Punto compensación
LO :	INIST-1151.354000069167050026
ID :	97-0487890

Links to Exploration step

Pascal:97-0487890

Le document en format XML

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Co<sub>11</sub>
B<sub>4</sub>
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Co<sub>11</sub>
B<sub>4</sub>
 compound</title>
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<term>Electron-electron interactions</term>
<term>Experimental study</term>
<term>Hexagonal lattices</term>
<term>Magnetic field effects</term>
<term>Magnetic hysteresis</term>
<term>Magnetization</term>
<term>Scattering</term>
<term>Spin waves</term>
<term>Ternary alloys</term>
<term>Thulium alloys</term>
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<keywords scheme="Pascal" xml:lang="fr"><term>Aimantation</term>
<term>Force coercitive</term>
<term>Conductivité électrique</term>
<term>Hystérésis magnétique</term>
<term>Effet champ magnétique</term>
<term>Réseau hexagonal</term>
<term>Point compensation</term>
<term>Interaction électron électron</term>
<term>Diffusion</term>
<term>Onde spin</term>
<term>Alliage base cobalt</term>
<term>Thulium alliage</term>
<term>Bore alliage</term>
<term>Alliage ternaire</term>
<term>Etude expérimentale</term>
<term>7560E</term>
<term>7215E</term>
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<front><div type="abstract" xml:lang="en">Copyright (c) 1997  Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound have been studied. This compound crystallizes in the hexagonal Ce<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 type structure. Results show that the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 is a ferromagnet with T<sub>C</sub>
=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T<sup>2</sup>
 dependence, implying that electron-spin wave scattering is dominant in this temperature range.</div>
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<fA08 i1="01" i2="1" l="ENG"><s1>Magnetic and electrical resistivity study of Tm<sub>3</sub>
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B<sub>4</sub>
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<fA11 i1="01" i2="1"><s1>KOWALCZYK (A.)</s1>
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<fA11 i1="02" i2="1"><s1>SMARDZ (L.)</s1>
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<fA14 i1="01"><s1>Institute of Molecular Physics, Polish Academy of Sciences, Smoluchowskiego 17, 60-179</s1>
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<sZ>2 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>Copyright (c) 1997  Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound have been studied. This compound crystallizes in the hexagonal Ce<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 type structure. Results show that the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 is a ferromagnet with T<sub>C</sub>
=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T<sup>2</sup>
 dependence, implying that electron-spin wave scattering is dominant in this temperature range.</s0>
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<fC02 i1="03" i2="X"><s0>240</s0>
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<fC03 i1="01" i2="3" l="FRE"><s0>Aimantation</s0>
<s5>02</s5>
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<fC03 i1="01" i2="3" l="ENG"><s0>Magnetization</s0>
<s5>02</s5>
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<fC03 i1="02" i2="3" l="FRE"><s0>Force coercitive</s0>
<s5>03</s5>
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<fC03 i1="02" i2="3" l="ENG"><s0>Coercive force</s0>
<s5>03</s5>
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<fC03 i1="03" i2="3" l="FRE"><s0>Conductivité électrique</s0>
<s5>04</s5>
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<fC03 i1="03" i2="3" l="ENG"><s0>Electric conductivity</s0>
<s5>04</s5>
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<fC03 i1="04" i2="X" l="FRE"><s0>Hystérésis magnétique</s0>
<s5>05</s5>
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<fC03 i1="04" i2="X" l="ENG"><s0>Magnetic hysteresis</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="GER"><s0>Magnetische Hysteresis</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Histérisis magnética</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Effet champ magnétique</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Magnetic field effects</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Réseau hexagonal</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Hexagonal lattices</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Point compensation</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Compensation point</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Punto compensación</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Interaction électron électron</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Electron-electron interactions</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Diffusion</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Scattering</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Onde spin</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Spin waves</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Alliage base cobalt</s0>
<s2>NK</s2>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Cobalt base alloys</s0>
<s2>NK</s2>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Thulium alliage</s0>
<s5>13</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Thulium alloys</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Bore alliage</s0>
<s5>14</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Boron alloys</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Alliage ternaire</s0>
<s5>15</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Ternary alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>18</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>18</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>7560E</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>7215E</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Alliage Co54Tm42B4</s0>
<s2>NK</s2>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>B Co Tm</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Lanthanide alliage</s0>
<s5>16</s5>
</fC07>
<fC07 i1="01" i2="3" l="ENG"><s0>Rare earth alloys</s0>
<s5>16</s5>
</fC07>
<fC07 i1="02" i2="3" l="FRE"><s0>Métal transition alliage</s0>
<s5>17</s5>
</fC07>
<fC07 i1="02" i2="3" l="ENG"><s0>Transition element alloys</s0>
<s5>17</s5>
</fC07>
<fN21><s1>300</s1>
</fN21>
</pA>
</standard>
<server><NO>PASCAL 97-0487890 Elsevier</NO>
<ET>Magnetic and electrical resistivity study of Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound</ET>
<AU>KOWALCZYK (A.); SMARDZ (L.)</AU>
<AF>Institute of Molecular Physics, Polish Academy of Sciences, Smoluchowskiego 17, 60-179/Poznań/Pologne (1 aut., 2 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Journal of alloys and compounds; ISSN 0925-8388; Suisse; Da. 1997; Vol. 259; Pp. 59-61; Abs. anglais</SO>
<LA>Anglais</LA>
<EA>Copyright (c) 1997  Elsevier Science S.A. All rights reserved. The magnetic (magnetization and coercivity) and transport (electrical resistivity) properties of the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound have been studied. This compound crystallizes in the hexagonal Ce<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 type structure. Results show that the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 is a ferromagnet with T<sub>C</sub>
=347 K and a compensation point equal to 125 K. The coercivity of the compound was determined from hysteresis measurements in fields up to 4 T. For the Tm<sub>3</sub>
Co<sub>11</sub>
B<sub>4</sub>
 compound we have observed a large increase of coercivity at low temperatures, typically from 0.01 T at 295 K to 0.8 T at 30 K. The resistivity at low temperatures shows a T<sup>2</sup>
 dependence, implying that electron-spin wave scattering is dominant in this temperature range.</EA>
<CC>001B70E60E; 001B70B15E; 240</CC>
<FD>Aimantation; Force coercitive; Conductivité électrique; Hystérésis magnétique; Effet champ magnétique; Réseau hexagonal; Point compensation; Interaction électron électron; Diffusion; Onde spin; Alliage base cobalt; Thulium alliage; Bore alliage; Alliage ternaire; Etude expérimentale; 7560E; 7215E; Alliage Co54Tm42B4; B Co Tm</FD>
<FG>Lanthanide alliage; Métal transition alliage</FG>
<ED>Magnetization; Coercive force; Electric conductivity; Magnetic hysteresis; Magnetic field effects; Hexagonal lattices; Compensation point; Electron-electron interactions; Scattering; Spin waves; Cobalt base alloys; Thulium alloys; Boron alloys; Ternary alloys; Experimental study</ED>
<EG>Rare earth alloys; Transition element alloys</EG>
<GD>Magnetische Hysteresis</GD>
<SD>Histérisis magnética; Punto compensación</SD>
<LO>INIST-1151.354000069167050026</LO>
<ID>97-0487890</ID>
</server>
</inist>
</record>

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Magnetic and electrical resistivity study of Tm3Co11B4 compound

Magnetic and electrical resistivity study of Tm3Co11B4 compound

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