ThuliumV1, Pascal, Corpus, bibRecord, 000E92

Magnetocrystalline anisotropy of Er2Fe14B and Tm2Fe14B at 4.2 K

Identifieur interne : 000E92 ( Pascal/Corpus ); précédent : 000E91; suivant : 000E93

Magnetocrystalline anisotropy of Er2Fe14B and Tm2Fe14B at 4.2 K

Auteurs : Y. B. Kima ; Jin Han-Min

Source :

Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2000.

RBID : Pascal:01-0057768

Descripteurs français

Pascal (Inist)
- Etude théorique, Anisotropie magnétique, Aimantation, Erbium alliage, Fer alliage, Bore alliage, Thulium alliage, Alliage ternaire, Alliage BErFe, Alliage BFeTm, B Fe Tm, B Er Fe, 7530G, 7550B.

English descriptors

KwdEn :
- Boron alloys, Erbium alloys, Iron alloys, Magnetic anisotropy, Magnetization, Ternary alloys, Theoretical study, Thulium alloys.

Abstract

The magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er₂Fe₁₄B and Tm₂Fe₁₄B at 4.2K have been determined as K_1Er = - 1255J/kg, K_3Er = - 30J/kg, N_ErFc = 0.43 T/Am² kg^-1 and K_1Tm = - 6830J/kg, K_3Tm = - 260J/kg, N_TmFe = 0.38 T/Am² kg^-1, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.

Notice en format standard (ISO 2709)

Pour connaître la documentation sur le format Inist Standard.

A01	`01`	`1`		`@0 0304-8853`
A02	`01`			`@0 JMMMDC`
A03		`1`		`@0 J. magn. magn. mater.`
A05				`@2 222`
A06				`@2 1-2`
A08	`01`	`1`	`ENG`	`@1 Magnetocrystalline anisotropy of Er₂Fe₁₄B and Tm₂Fe₁₄B at 4.2 K`
A11	`01`	`1`		`@1 KIMA (Y. B.)`
A11	`02`	`1`		`@1 HAN-MIN (Jin)`
A14	`01`			`@1 Korea Research Institute of Standards and Science, P. O. Box 3 @2 Taejon 305-600 @3 KOR @Z 1 aut.`
A14	`02`			`@1 Jilin University @2 Changchun @3 CHN @Z 2 aut.`
A20				`@1 39-46`
A21				`@1 2000`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 17230 @5 354000093753540060`
A44				`@0 0000 @1 © 2001 INIST-CNRS. All rights reserved.`
A45				`@0 14 ref.`
A47	`01`	`1`		`@0 01-0057768`
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 magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er₂Fe₁₄B and Tm₂Fe₁₄B at 4.2K have been determined as K_1Er = - 1255J/kg, K_3Er = - 30J/kg, N_ErFc = 0.43 T/Am² kg^-1 and K_1Tm = - 6830J/kg, K_3Tm = - 260J/kg, N_TmFe = 0.38 T/Am² kg^-1, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.
C02	`01`	`3`		`@0 001B70E30G`
C02	`02`	`3`		`@0 001B70E50B`
C02	`03`	`X`		`@0 240`
C03	`01`	`3`	`FRE`	`@0 Etude théorique @5 01`
C03	`01`	`3`	`ENG`	`@0 Theoretical study @5 01`
C03	`02`	`3`	`FRE`	`@0 Anisotropie magnétique @5 02`
C03	`02`	`3`	`ENG`	`@0 Magnetic anisotropy @5 02`
C03	`03`	`3`	`FRE`	`@0 Aimantation @5 03`
C03	`03`	`3`	`ENG`	`@0 Magnetization @5 03`
C03	`04`	`3`	`FRE`	`@0 Erbium alliage @5 04`
C03	`04`	`3`	`ENG`	`@0 Erbium alloys @5 04`
C03	`05`	`3`	`FRE`	`@0 Fer alliage @5 05`
C03	`05`	`3`	`ENG`	`@0 Iron alloys @5 05`
C03	`06`	`3`	`FRE`	`@0 Bore alliage @5 06`
C03	`06`	`3`	`ENG`	`@0 Boron alloys @5 06`
C03	`07`	`3`	`FRE`	`@0 Thulium alliage @5 07`
C03	`07`	`3`	`ENG`	`@0 Thulium alloys @5 07`
C03	`08`	`3`	`FRE`	`@0 Alliage ternaire @5 08`
C03	`08`	`3`	`ENG`	`@0 Ternary alloys @5 08`
C03	`09`	`3`	`FRE`	`@0 Alliage BErFe @2 NK @4 INC @5 52`
C03	`10`	`3`	`FRE`	`@0 Alliage BFeTm @2 NK @4 INC @5 53`
C03	`11`	`3`	`FRE`	`@0 B Fe Tm @4 INC @5 54`
C03	`12`	`3`	`FRE`	`@0 B Er Fe @4 INC @5 55`
C03	`13`	`3`	`FRE`	`@0 7530G @2 PAC @4 INC @5 56`
C03	`14`	`3`	`FRE`	`@0 7550B @2 PAC @4 INC @5 57`
C07	`01`	`3`	`FRE`	`@0 Métal transition alliage @5 48`
C07	`01`	`3`	`ENG`	`@0 Transition element alloys @5 48`
C07	`02`	`3`	`FRE`	`@0 Lanthanide alliage @5 49`
C07	`02`	`3`	`ENG`	`@0 Rare earth alloys @5 49`
N21				`@1 036`

Format Inist (serveur)

NO :	PASCAL 01-0057768 INIST
ET :	Magnetocrystalline anisotropy of Er₂Fe₁₄B and Tm₂Fe₁₄B at 4.2 K
AU :	KIMA (Y. B.); HAN-MIN (Jin)
AF :	Korea Research Institute of Standards and Science, P. O. Box 3/Taejon 305-600/Corée, République de (1 aut.); Jilin University/Changchun/Chine (2 aut.)
DT :	Publication en série; Niveau analytique
SO :	Journal of magnetism and magnetic materials; ISSN 0304-8853; Coden JMMMDC; Pays-Bas; Da. 2000; Vol. 222; No. 1-2; Pp. 39-46; Bibl. 14 ref.
LA :	Anglais
EA :	The magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er₂Fe₁₄B and Tm₂Fe₁₄B at 4.2K have been determined as K_1Er = - 1255J/kg, K_3Er = - 30J/kg, N_ErFc = 0.43 T/Am² kg^-1 and K_1Tm = - 6830J/kg, K_3Tm = - 260J/kg, N_TmFe = 0.38 T/Am² kg^-1, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.
CC :	001B70E30G; 001B70E50B; 240
FD :	Etude théorique; Anisotropie magnétique; Aimantation; Erbium alliage; Fer alliage; Bore alliage; Thulium alliage; Alliage ternaire; Alliage BErFe; Alliage BFeTm; B Fe Tm; B Er Fe; 7530G; 7550B
FG :	Métal transition alliage; Lanthanide alliage
ED :	Theoretical study; Magnetic anisotropy; Magnetization; Erbium alloys; Iron alloys; Boron alloys; Thulium alloys; Ternary alloys
EG :	Transition element alloys; Rare earth alloys
LO :	INIST-17230.354000093753540060
ID :	01-0057768

Links to Exploration step

Pascal:01-0057768

Le document en format XML

<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Magnetocrystalline anisotropy of Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2 K</title>
<author><name sortKey="Kima, Y B" sort="Kima, Y B" uniqKey="Kima Y" first="Y. B." last="Kima">Y. B. Kima</name>
<affiliation><inist:fA14 i1="01"><s1>Korea Research Institute of Standards and Science, P. O. Box 3</s1>
<s2>Taejon 305-600</s2>
<s3>KOR</s3>
<sZ>1 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Han Min, Jin" sort="Han Min, Jin" uniqKey="Han Min J" first="Jin" last="Han-Min">Jin Han-Min</name>
<affiliation><inist:fA14 i1="02"><s1>Jilin University</s1>
<s2>Changchun</s2>
<s3>CHN</s3>
<sZ>2 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
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<idno type="stanalyst">PASCAL 01-0057768 INIST</idno>
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<idno type="wicri:Area/Pascal/Corpus">000E92</idno>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetocrystalline anisotropy of Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2 K</title>
<author><name sortKey="Kima, Y B" sort="Kima, Y B" uniqKey="Kima Y" first="Y. B." last="Kima">Y. B. Kima</name>
<affiliation><inist:fA14 i1="01"><s1>Korea Research Institute of Standards and Science, P. O. Box 3</s1>
<s2>Taejon 305-600</s2>
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<sZ>1 aut.</sZ>
</inist:fA14>
</affiliation>
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<author><name sortKey="Han Min, Jin" sort="Han Min, Jin" uniqKey="Han Min J" first="Jin" last="Han-Min">Jin Han-Min</name>
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<series><title level="j" type="main">Journal of magnetism and magnetic materials</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Boron alloys</term>
<term>Erbium alloys</term>
<term>Iron alloys</term>
<term>Magnetic anisotropy</term>
<term>Magnetization</term>
<term>Ternary alloys</term>
<term>Theoretical study</term>
<term>Thulium alloys</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude théorique</term>
<term>Anisotropie magnétique</term>
<term>Aimantation</term>
<term>Erbium alliage</term>
<term>Fer alliage</term>
<term>Bore alliage</term>
<term>Thulium alliage</term>
<term>Alliage ternaire</term>
<term>Alliage BErFe</term>
<term>Alliage BFeTm</term>
<term>B Fe Tm</term>
<term>B Er Fe</term>
<term>7530G</term>
<term>7550B</term>
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<front><div type="abstract" xml:lang="en">The magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2K have been determined as K<sub>1Er</sub>
 = - 1255J/kg, K<sub>3Er</sub>
 = - 30J/kg, N<sub>ErFc</sub>
 = 0.43 T/Am<sup>2</sup>
 kg<sup>-1</sup>
 and K<sub>1Tm</sub>
 = - 6830J/kg, K<sub>3Tm</sub>
 = - 260J/kg, N<sub>TmFe</sub>
 = 0.38 T/Am<sup>2</sup>
 kg<sup>-1</sup>
, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.</div>
</front>
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B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2 K</s1>
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<fA14 i1="01"><s1>Korea Research Institute of Standards and Science, P. O. Box 3</s1>
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<sZ>1 aut.</sZ>
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<fA14 i1="02"><s1>Jilin University</s1>
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<fC01 i1="01" l="ENG"><s0>The magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2K have been determined as K<sub>1Er</sub>
 = - 1255J/kg, K<sub>3Er</sub>
 = - 30J/kg, N<sub>ErFc</sub>
 = 0.43 T/Am<sup>2</sup>
 kg<sup>-1</sup>
 and K<sub>1Tm</sub>
 = - 6830J/kg, K<sub>3Tm</sub>
 = - 260J/kg, N<sub>TmFe</sub>
 = 0.38 T/Am<sup>2</sup>
 kg<sup>-1</sup>
, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E30G</s0>
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<s5>01</s5>
</fC03>
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<s5>02</s5>
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<s5>03</s5>
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<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Erbium alliage</s0>
<s5>04</s5>
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<s5>04</s5>
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<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Iron alloys</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Bore alliage</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Boron alloys</s0>
<s5>06</s5>
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<s5>07</s5>
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<s5>07</s5>
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<s5>08</s5>
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<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Alliage BErFe</s0>
<s2>NK</s2>
<s4>INC</s4>
<s5>52</s5>
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<s2>NK</s2>
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<s5>53</s5>
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<s5>54</s5>
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<s4>INC</s4>
<s5>55</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>7530G</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>7550B</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
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<s5>48</s5>
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<s5>48</s5>
</fC07>
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<s5>49</s5>
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<server><NO>PASCAL 01-0057768 INIST</NO>
<ET>Magnetocrystalline anisotropy of Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2 K</ET>
<AU>KIMA (Y. B.); HAN-MIN (Jin)</AU>
<AF>Korea Research Institute of Standards and Science, P. O. Box 3/Taejon 305-600/Corée, République de (1 aut.); Jilin University/Changchun/Chine (2 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Journal of magnetism and magnetic materials; ISSN 0304-8853; Coden JMMMDC; Pays-Bas; Da. 2000; Vol. 222; No. 1-2; Pp. 39-46; Bibl. 14 ref.</SO>
<LA>Anglais</LA>
<EA>The magnetization process of in-plane anisotropy system with tetragonal structure has been examined on the basis of rigid coupled magnetization and two sublattice magnetization models. By applying graphical and fitting methods, the magnetocrystalline anisotropy constant sets for Er<sub>2</sub>
Fe<sub>14</sub>
B and Tm<sub>2</sub>
Fe<sub>14</sub>
B at 4.2K have been determined as K<sub>1Er</sub>
 = - 1255J/kg, K<sub>3Er</sub>
 = - 30J/kg, N<sub>ErFc</sub>
 = 0.43 T/Am<sup>2</sup>
 kg<sup>-1</sup>
 and K<sub>1Tm</sub>
 = - 6830J/kg, K<sub>3Tm</sub>
 = - 260J/kg, N<sub>TmFe</sub>
 = 0.38 T/Am<sup>2</sup>
 kg<sup>-1</sup>
, respectively. The magnetizations calculated by energy minimum method by applying the anisotropy constant sets reproduced well the experiments and satisfied the simulation assumptions.</EA>
<CC>001B70E30G; 001B70E50B; 240</CC>
<FD>Etude théorique; Anisotropie magnétique; Aimantation; Erbium alliage; Fer alliage; Bore alliage; Thulium alliage; Alliage ternaire; Alliage BErFe; Alliage BFeTm; B Fe Tm; B Er Fe; 7530G; 7550B</FD>
<FG>Métal transition alliage; Lanthanide alliage</FG>
<ED>Theoretical study; Magnetic anisotropy; Magnetization; Erbium alloys; Iron alloys; Boron alloys; Thulium alloys; Ternary alloys</ED>
<EG>Transition element alloys; Rare earth alloys</EG>
<LO>INIST-17230.354000093753540060</LO>
<ID>01-0057768</ID>
</server>
</inist>
</record>

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Magnetocrystalline anisotropy of Er2Fe14B and Tm2Fe14B at 4.2 K

Magnetocrystalline anisotropy of Er2Fe14B and Tm2Fe14B at 4.2 K

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