ThuliumV1, Pascal, Curation, bibRecord, 000588

Anisotropic magnetization of the Van Vleck paramagnet LiTmF4at low temperatures and high magnetic fields

Identifieur interne : 000588 ( Pascal/Curation ); précédent : 000587; suivant : 000589

Anisotropic magnetization of the Van Vleck paramagnet LiTmF4at low temperatures and high magnetic fields

Auteurs : D. I. Abubakirov [Russie, Japon] ; K. Matsumoto [Japon] ; H. Suzuki [Japon] ; M. S. Tagirov [Russie]

Source :

Journal of physics. Condensed matter : (Print) [ 0953-8984 ] ; 2008.

RBID : Pascal:08-0486998

Descripteurs français

Pascal (Inist)
- Anisotropie, Aimantation, Champ intense, Effet champ magnétique, Orientation champ, Variation angulaire, Effet température, Lithium Thulium Fluorure Mixte, Basse température, Matériau paramagnétique, Réseau quadratique, Monocristal.

English descriptors

KwdEn :
- Angular variation, Anisotropy, Field orientation, High field, Lithium Thulium Fluorides Mixed, Low temperature, Magnetic field effects, Magnetization, Monocrystals, Paramagnetic materials, Temperature effects, Tetragonal lattices.

Abstract

Lithium thulium fluoride LiTmF₄ is an insulating Van Vleck paramagnet with a giant magnetostriction. Magnetization of the tetragonal LiTmF₄ single crystals was measured for the first time in the temperature range of 2-300 K and in magnetic fields up to 55 kOe, oriented both parallel and perpendicular to the C₄ symmetry axis. In particular the angular dependence of the magnetization in the basal plane was studied. The anisotropy of magnetization in this plane grows rapidly in high fields. The temperature dependence of the magnetization in the orientation H ⁄ [001] is nonmonotonic and reproduced very well by the calculation in the framework of the crystal field theory. The discrepancies between experimental and theoretical dependences in the orientation H ⊥ [001] in high magnetic fields are attributed to the magnetostriction effects.

A01	`01`	`1`		`@0 0953-8984`
A02	`01`			`@0 JCOMEL`
A03		`1`		`@0 J. phys., Condens. matter : (Print)`
A05				`@2 20`
A06				`@2 39`
A08	`01`	`1`	`ENG`	`@1 Anisotropic magnetization of the Van Vleck paramagnet LiTmF₄at low temperatures and high magnetic fields`
A11	`01`	`1`		`@1 ABUBAKIROV (D. I.)`
A11	`02`	`1`		`@1 MATSUMOTO (K.)`
A11	`03`	`1`		`@1 SUZUKI (H.)`
A11	`04`	`1`		`@1 TAGIROV (M. S.)`
A14	`01`			`@1 Physics Department, Kazan State University, Kremlevskaya street, 18 @2 Kazan 420008 @3 RUS @Z 1 aut. @Z 4 aut.`
A14	`02`			`@1 Department of Physics, Kanazawa University @2 Kakuma-machi, Kanazawa 920-1192 @3 JPN @Z 1 aut. @Z 2 aut. @Z 3 aut.`
A20				`@2 395223.1-395223.4`
A21				`@1 2008`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 577E2 @5 354000185831700300`
A44				`@0 0000 @1 © 2008 INIST-CNRS. All rights reserved.`
A45				`@0 10 ref.`
A47	`01`	`1`		`@0 08-0486998`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of physics. Condensed matter : (Print)`
A66	`01`			`@0 GBR`
C01	`01`		`ENG`	@0 Lithium thulium fluoride LiTmF₄ is an insulating Van Vleck paramagnet with a giant magnetostriction. Magnetization of the tetragonal LiTmF₄ single crystals was measured for the first time in the temperature range of 2-300 K and in magnetic fields up to 55 kOe, oriented both parallel and perpendicular to the C₄ symmetry axis. In particular the angular dependence of the magnetization in the basal plane was studied. The anisotropy of magnetization in this plane grows rapidly in high fields. The temperature dependence of the magnetization in the orientation H ⁄ [001] is nonmonotonic and reproduced very well by the calculation in the framework of the crystal field theory. The discrepancies between experimental and theoretical dependences in the orientation H ⊥ [001] in high magnetic fields are attributed to the magnetostriction effects.
C02	`01`	`3`		`@0 001B70E20C`
C03	`01`	`3`	`FRE`	`@0 Anisotropie @5 02`
C03	`01`	`3`	`ENG`	`@0 Anisotropy @5 02`
C03	`02`	`3`	`FRE`	`@0 Aimantation @5 03`
C03	`02`	`3`	`ENG`	`@0 Magnetization @5 03`
C03	`03`	`3`	`FRE`	`@0 Champ intense @5 04`
C03	`03`	`3`	`ENG`	`@0 High field @5 04`
C03	`04`	`3`	`FRE`	`@0 Effet champ magnétique @5 05`
C03	`04`	`3`	`ENG`	`@0 Magnetic field effects @5 05`
C03	`05`	`X`	`FRE`	`@0 Orientation champ @5 06`
C03	`05`	`X`	`ENG`	`@0 Field orientation @5 06`
C03	`05`	`X`	`SPA`	`@0 Orientacíon campo @5 06`
C03	`06`	`X`	`FRE`	`@0 Variation angulaire @5 07`
C03	`06`	`X`	`ENG`	`@0 Angular variation @5 07`
C03	`06`	`X`	`SPA`	`@0 Variación angular @5 07`
C03	`07`	`3`	`FRE`	`@0 Effet température @5 09`
C03	`07`	`3`	`ENG`	`@0 Temperature effects @5 09`
C03	`08`	`X`	`FRE`	`@0 Lithium Thulium Fluorure Mixte @2 NC @2 NA @5 11`
C03	`08`	`X`	`ENG`	`@0 Lithium Thulium Fluorides Mixed @2 NC @2 NA @5 11`
C03	`08`	`X`	`SPA`	`@0 Mixto @2 NC @2 NA @5 11`
C03	`09`	`X`	`FRE`	`@0 Basse température @5 12`
C03	`09`	`X`	`ENG`	`@0 Low temperature @5 12`
C03	`09`	`X`	`SPA`	`@0 Baja temperatura @5 12`
C03	`10`	`3`	`FRE`	`@0 Matériau paramagnétique @5 15`
C03	`10`	`3`	`ENG`	`@0 Paramagnetic materials @5 15`
C03	`11`	`3`	`FRE`	`@0 Réseau quadratique @5 17`
C03	`11`	`3`	`ENG`	`@0 Tetragonal lattices @5 17`
C03	`12`	`3`	`FRE`	`@0 Monocristal @5 18`
C03	`12`	`3`	`ENG`	`@0 Monocrystals @5 18`
N21				`@1 316`

Links toward previous steps (curation, corpus...)

to stream Pascal, to step Corpus: Pour aller vers cette notice dans l'étape Curation :000588

Links to Exploration step

Pascal:08-0486998

Le document en format XML

<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Anisotropic magnetization of the Van Vleck paramagnet LiTmF<sub>4</sub>
at low temperatures and high magnetic fields</title>
<author><name sortKey="Abubakirov, D I" sort="Abubakirov, D I" uniqKey="Abubakirov D" first="D. I." last="Abubakirov">D. I. Abubakirov</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Physics Department, Kazan State University, Kremlevskaya street, 18</s1>
<s2>Kazan 420008</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Matsumoto, K" sort="Matsumoto, K" uniqKey="Matsumoto K" first="K." last="Matsumoto">K. Matsumoto</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Suzuki, H" sort="Suzuki, H" uniqKey="Suzuki H" first="H." last="Suzuki">H. Suzuki</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Tagirov, M S" sort="Tagirov, M S" uniqKey="Tagirov M" first="M. S." last="Tagirov">M. S. Tagirov</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Physics Department, Kazan State University, Kremlevskaya street, 18</s1>
<s2>Kazan 420008</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
</author>
</titleStmt>
<publicationStmt><idno type="wicri:source">INIST</idno>
<idno type="inist">08-0486998</idno>
<date when="2008">2008</date>
<idno type="stanalyst">PASCAL 08-0486998 INIST</idno>
<idno type="RBID">Pascal:08-0486998</idno>
<idno type="wicri:Area/Pascal/Corpus">000588</idno>
<idno type="wicri:Area/Pascal/Curation">000588</idno>
</publicationStmt>
<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Anisotropic magnetization of the Van Vleck paramagnet LiTmF<sub>4</sub>
at low temperatures and high magnetic fields</title>
<author><name sortKey="Abubakirov, D I" sort="Abubakirov, D I" uniqKey="Abubakirov D" first="D. I." last="Abubakirov">D. I. Abubakirov</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Physics Department, Kazan State University, Kremlevskaya street, 18</s1>
<s2>Kazan 420008</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Matsumoto, K" sort="Matsumoto, K" uniqKey="Matsumoto K" first="K." last="Matsumoto">K. Matsumoto</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Suzuki, H" sort="Suzuki, H" uniqKey="Suzuki H" first="H." last="Suzuki">H. Suzuki</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>Japon</country>
</affiliation>
</author>
<author><name sortKey="Tagirov, M S" sort="Tagirov, M S" uniqKey="Tagirov M" first="M. S." last="Tagirov">M. S. Tagirov</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Physics Department, Kazan State University, Kremlevskaya street, 18</s1>
<s2>Kazan 420008</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Russie</country>
</affiliation>
</author>
</analytic>
<series><title level="j" type="main">Journal of physics. Condensed matter : (Print)</title>
<title level="j" type="abbreviated">J. phys., Condens. matter : (Print)</title>
<idno type="ISSN">0953-8984</idno>
<imprint><date when="2008">2008</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Journal of physics. Condensed matter : (Print)</title>
<title level="j" type="abbreviated">J. phys., Condens. matter : (Print)</title>
<idno type="ISSN">0953-8984</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Angular variation</term>
<term>Anisotropy</term>
<term>Field orientation</term>
<term>High field</term>
<term>Lithium Thulium Fluorides Mixed</term>
<term>Low temperature</term>
<term>Magnetic field effects</term>
<term>Magnetization</term>
<term>Monocrystals</term>
<term>Paramagnetic materials</term>
<term>Temperature effects</term>
<term>Tetragonal lattices</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Anisotropie</term>
<term>Aimantation</term>
<term>Champ intense</term>
<term>Effet champ magnétique</term>
<term>Orientation champ</term>
<term>Variation angulaire</term>
<term>Effet température</term>
<term>Lithium Thulium Fluorure Mixte</term>
<term>Basse température</term>
<term>Matériau paramagnétique</term>
<term>Réseau quadratique</term>
<term>Monocristal</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Lithium thulium fluoride LiTmF<sub>4</sub>
 is an insulating Van Vleck paramagnet with a giant magnetostriction. Magnetization of the tetragonal LiTmF<sub>4</sub>
 single crystals was measured for the first time in the temperature range of 2-300 K and in magnetic fields up to 55 kOe, oriented both parallel and perpendicular to the C<sub>4</sub>
 symmetry axis. In particular the angular dependence of the magnetization in the basal plane was studied. The anisotropy of magnetization in this plane grows rapidly in high fields. The temperature dependence of the magnetization in the orientation H ⁄ [001] is nonmonotonic and reproduced very well by the calculation in the framework of the crystal field theory. The discrepancies between experimental and theoretical dependences in the orientation H ⊥ [001] in high magnetic fields are attributed to the magnetostriction effects.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0953-8984</s0>
</fA01>
<fA02 i1="01"><s0>JCOMEL</s0>
</fA02>
<fA03 i2="1"><s0>J. phys., Condens. matter : (Print)</s0>
</fA03>
<fA05><s2>20</s2>
</fA05>
<fA06><s2>39</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Anisotropic magnetization of the Van Vleck paramagnet LiTmF<sub>4</sub>
at low temperatures and high magnetic fields</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>ABUBAKIROV (D. I.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>MATSUMOTO (K.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>SUZUKI (H.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>TAGIROV (M. S.)</s1>
</fA11>
<fA14 i1="01"><s1>Physics Department, Kazan State University, Kremlevskaya street, 18</s1>
<s2>Kazan 420008</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Department of Physics, Kanazawa University</s1>
<s2>Kakuma-machi, Kanazawa 920-1192</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14>
<fA20><s2>395223.1-395223.4</s2>
</fA20>
<fA21><s1>2008</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>577E2</s2>
<s5>354000185831700300</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2008 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>10 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>08-0486998</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
</fA61>
<fA64 i1="01" i2="1"><s0>Journal of physics. Condensed matter : (Print)</s0>
</fA64>
<fA66 i1="01"><s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>Lithium thulium fluoride LiTmF<sub>4</sub>
 is an insulating Van Vleck paramagnet with a giant magnetostriction. Magnetization of the tetragonal LiTmF<sub>4</sub>
 single crystals was measured for the first time in the temperature range of 2-300 K and in magnetic fields up to 55 kOe, oriented both parallel and perpendicular to the C<sub>4</sub>
 symmetry axis. In particular the angular dependence of the magnetization in the basal plane was studied. The anisotropy of magnetization in this plane grows rapidly in high fields. The temperature dependence of the magnetization in the orientation H ⁄ [001] is nonmonotonic and reproduced very well by the calculation in the framework of the crystal field theory. The discrepancies between experimental and theoretical dependences in the orientation H ⊥ [001] in high magnetic fields are attributed to the magnetostriction effects.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70E20C</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Anisotropie</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Anisotropy</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Aimantation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Magnetization</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Champ intense</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>High field</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Effet champ magnétique</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Magnetic field effects</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Orientation champ</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Field orientation</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Orientacíon campo</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Variation angulaire</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Angular variation</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Variación angular</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Effet température</s0>
<s5>09</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Temperature effects</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Lithium Thulium Fluorure Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Lithium Thulium Fluorides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Mixto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Basse température</s0>
<s5>12</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Low temperature</s0>
<s5>12</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Baja temperatura</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Matériau paramagnétique</s0>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Paramagnetic materials</s0>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Réseau quadratique</s0>
<s5>17</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Tetragonal lattices</s0>
<s5>17</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Monocristal</s0>
<s5>18</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Monocrystals</s0>
<s5>18</s5>
</fC03>
<fN21><s1>316</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

Pour manipuler ce document sous Unix (Dilib)

EXPLOR_STEP=$WICRI_ROOT/Wicri/Terre/explor/ThuliumV1/Data/Pascal/Curation

HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 000588 | SxmlIndent | more

HfdSelect -h $EXPLOR_AREA/Data/Pascal/Curation/biblio.hfd -nk 000588 | SxmlIndent | more

Pour mettre un lien sur cette page dans le réseau Wicri

{{Explor lien
   |wiki=    Wicri/Terre
   |area=    ThuliumV1
   |flux=    Pascal
   |étape=   Curation
   |type=    RBID
   |clé=     Pascal:08-0486998
   |texte=   Anisotropic magnetization of the Van Vleck paramagnet LiTmF4at low temperatures and high magnetic fields
}}

This area was generated with Dilib version V0.6.21.
Data generation: Thu May 12 08:27:09 2016. Site generation: Thu Mar 7 22:33:44 2024

	Serveur d'exploration sur le thulium
	Attention, ce site est en cours de développement ! Attention, site généré par des moyens informatiques à partir de corpus bruts. Les informations ne sont donc pas validées.

Serveur d'exploration sur le thulium

Anisotropic magnetization of the Van Vleck paramagnet LiTmF4at low temperatures and high magnetic fields

Anisotropic magnetization of the Van Vleck paramagnet LiTmF4at low temperatures and high magnetic fields

Source :

Descripteurs français

English descriptors

Abstract

Links toward previous steps (curation, corpus...)

Links to Exploration step

Le document en format XML

Pour manipuler ce document sous Unix (Dilib)

Pour mettre un lien sur cette page dans le réseau Wicri