Magnetic structure of TmCu2Ge2
Identifieur interne : 000153 ( Pascal/Corpus ); précédent : 000152; suivant : 000154Magnetic structure of TmCu2Ge2
Auteurs : B. Penc ; S. Gerischer ; A. Hoser ; A. SzytulaSource :
- Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2012.
Descripteurs français
- Pascal (Inist)
English descriptors
- KwdEn :
Abstract
TmCu2Ge2 compound crystallizes in the tetragonal ThCr2Si2-type crystal structure. The neutron diffraction reveals the presence of an incommensurate antiferromagnetic order below TN=2.5 K. The Tm magnetic moment of 5.0(1) μB at 0.47 K is parallel to the c-axis. The order is described by the propagation vector k=[kx, kx, 0], where kx=0.117(3). The increase of the values of the components kx near the Néel temperature is observed.
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Format Inist (serveur)
NO : | PASCAL 12-0237219 INIST |
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ET : | Magnetic structure of TmCu2Ge2 |
AU : | PENC (B.); GERISCHER (S.); HOSER (A.); SZYTULA (A.) |
AF : | M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4/30-059 Kraków/Pologne (1 aut., 4 aut.); BENSC, Helmholtz-Zentrum Berlin, Hahn-Meitner-Platz 1/14 109 Berlin/Allemagne (2 aut., 3 aut.) |
DT : | Publication en série; Lettre à l'éditeur; Niveau analytique |
SO : | Journal of magnetism and magnetic materials; ISSN 0304-8853; Coden JMMMDC; Pays-Bas; Da. 2012; Vol. 324; No. 5; Pp. 657-659; Bibl. 20 ref. |
LA : | Anglais |
EA : | TmCu2Ge2 compound crystallizes in the tetragonal ThCr2Si2-type crystal structure. The neutron diffraction reveals the presence of an incommensurate antiferromagnetic order below TN=2.5 K. The Tm magnetic moment of 5.0(1) μB at 0.47 K is parallel to the c-axis. The order is described by the propagation vector k=[kx, kx, 0], where kx=0.117(3). The increase of the values of the components kx near the Néel temperature is observed. |
CC : | 001B70E25 |
FD : | Structure magnétique; Structure cristalline; Diffraction neutron; Phase incommensurable; Antiferromagnétisme; Moment magnétique; Point Néel; Effet température; Cuivre Thulium Germaniure Mixte; Réseau quadratique |
ED : | Magnetic structure; Crystal structure; Neutron diffraction; Incommensurate phases; Antiferromagnetism; Magnetic moments; Neel temperature; Temperature effects; Copper Thulium Germanides Mixed; Tetragonal lattices |
SD : | Mixto |
LO : | INIST-17230.354000509349920010 |
ID : | 12-0237219 |
Links to Exploration step
Pascal:12-0237219Le document en format XML
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Ge<sub>2</sub>
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<author><name sortKey="Penc, B" sort="Penc, B" uniqKey="Penc B" first="B." last="Penc">B. Penc</name>
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<s2>30-059 Kraków</s2>
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<author><name sortKey="Gerischer, S" sort="Gerischer, S" uniqKey="Gerischer S" first="S." last="Gerischer">S. Gerischer</name>
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Ge<sub>2</sub>
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<author><name sortKey="Hoser, A" sort="Hoser, A" uniqKey="Hoser A" first="A." last="Hoser">A. Hoser</name>
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<series><title level="j" type="main">Journal of magnetism and magnetic materials</title>
<title level="j" type="abbreviated">J. magn. magn. mater.</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Antiferromagnetism</term>
<term>Copper Thulium Germanides Mixed</term>
<term>Crystal structure</term>
<term>Incommensurate phases</term>
<term>Magnetic moments</term>
<term>Magnetic structure</term>
<term>Neel temperature</term>
<term>Neutron diffraction</term>
<term>Temperature effects</term>
<term>Tetragonal lattices</term>
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<term>Structure cristalline</term>
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<term>Antiferromagnétisme</term>
<term>Moment magnétique</term>
<term>Point Néel</term>
<term>Effet température</term>
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<front><div type="abstract" xml:lang="en">TmCu<sub>2</sub>
Ge<sub>2</sub>
compound crystallizes in the tetragonal ThCr<sub>2</sub>
Si<sub>2</sub>
-type crystal structure. The neutron diffraction reveals the presence of an incommensurate antiferromagnetic order below T<sub>N</sub>
=2.5 K. The Tm magnetic moment of 5.0(1) μB at 0.47 K is parallel to the c-axis. The order is described by the propagation vector k=[k<sub>x</sub>
, k<sub>x</sub>
, 0], where k<sub>x</sub>
=0.117(3). The increase of the values of the components k<sub>x</sub>
near the Néel temperature is observed.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Magnetic structure of TmCu<sub>2</sub>
Ge<sub>2</sub>
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<fA11 i1="01" i2="1"><s1>PENC (B.)</s1>
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<s3>POL</s3>
<sZ>1 aut.</sZ>
<sZ>4 aut.</sZ>
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<fA14 i1="02"><s1>BENSC, Helmholtz-Zentrum Berlin, Hahn-Meitner-Platz 1</s1>
<s2>14 109 Berlin</s2>
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<sZ>2 aut.</sZ>
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<fA45><s0>20 ref.</s0>
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<fA47 i1="01" i2="1"><s0>12-0237219</s0>
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<fA60><s1>P</s1>
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<fC01 i1="01" l="ENG"><s0>TmCu<sub>2</sub>
Ge<sub>2</sub>
compound crystallizes in the tetragonal ThCr<sub>2</sub>
Si<sub>2</sub>
-type crystal structure. The neutron diffraction reveals the presence of an incommensurate antiferromagnetic order below T<sub>N</sub>
=2.5 K. The Tm magnetic moment of 5.0(1) μB at 0.47 K is parallel to the c-axis. The order is described by the propagation vector k=[k<sub>x</sub>
, k<sub>x</sub>
, 0], where k<sub>x</sub>
=0.117(3). The increase of the values of the components k<sub>x</sub>
near the Néel temperature is observed.</s0>
</fC01>
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<s5>02</s5>
</fC03>
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<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Crystal structure</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Diffraction neutron</s0>
<s5>04</s5>
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<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Incommensurate phases</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Antiferromagnétisme</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Antiferromagnetism</s0>
<s5>06</s5>
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<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Magnetic moments</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Point Néel</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Neel temperature</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Effet température</s0>
<s5>09</s5>
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<fC03 i1="09" i2="X" l="FRE"><s0>Cuivre Thulium Germaniure Mixte</s0>
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<s2>NC</s2>
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<fC03 i1="09" i2="X" l="SPA"><s0>Mixto</s0>
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<s2>NA</s2>
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<fC03 i1="10" i2="3" l="FRE"><s0>Réseau quadratique</s0>
<s5>15</s5>
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<fN21><s1>184</s1>
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<server><NO>PASCAL 12-0237219 INIST</NO>
<ET>Magnetic structure of TmCu<sub>2</sub>
Ge<sub>2</sub>
</ET>
<AU>PENC (B.); GERISCHER (S.); HOSER (A.); SZYTULA (A.)</AU>
<AF>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4/30-059 Kraków/Pologne (1 aut., 4 aut.); BENSC, Helmholtz-Zentrum Berlin, Hahn-Meitner-Platz 1/14 109 Berlin/Allemagne (2 aut., 3 aut.)</AF>
<DT>Publication en série; Lettre à l'éditeur; Niveau analytique</DT>
<SO>Journal of magnetism and magnetic materials; ISSN 0304-8853; Coden JMMMDC; Pays-Bas; Da. 2012; Vol. 324; No. 5; Pp. 657-659; Bibl. 20 ref.</SO>
<LA>Anglais</LA>
<EA>TmCu<sub>2</sub>
Ge<sub>2</sub>
compound crystallizes in the tetragonal ThCr<sub>2</sub>
Si<sub>2</sub>
-type crystal structure. The neutron diffraction reveals the presence of an incommensurate antiferromagnetic order below T<sub>N</sub>
=2.5 K. The Tm magnetic moment of 5.0(1) μB at 0.47 K is parallel to the c-axis. The order is described by the propagation vector k=[k<sub>x</sub>
, k<sub>x</sub>
, 0], where k<sub>x</sub>
=0.117(3). The increase of the values of the components k<sub>x</sub>
near the Néel temperature is observed.</EA>
<CC>001B70E25</CC>
<FD>Structure magnétique; Structure cristalline; Diffraction neutron; Phase incommensurable; Antiferromagnétisme; Moment magnétique; Point Néel; Effet température; Cuivre Thulium Germaniure Mixte; Réseau quadratique</FD>
<ED>Magnetic structure; Crystal structure; Neutron diffraction; Incommensurate phases; Antiferromagnetism; Magnetic moments; Neel temperature; Temperature effects; Copper Thulium Germanides Mixed; Tetragonal lattices</ED>
<SD>Mixto</SD>
<LO>INIST-17230.354000509349920010</LO>
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