Magnetic behavior in TmAgSi
Identifieur interne : 000299 ( Pascal/Curation ); précédent : 000298; suivant : 000300Magnetic behavior in TmAgSi
Auteurs : S. Baran [Pologne] ; D. Kaczorowski [Pologne] ; A. Hoser [Allemagne] ; B. Penc [Pologne] ; A. Szytula [Pologne]Source :
- Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2011.
Descripteurs français
- Pascal (Inist)
- Structure cristalline, Chaleur massique, Diffraction neutron, Antiferromagnétisme, Moment magnétique, Structure magnétique, Ferromagnétisme, Structure spin incliné, Interaction RKKY, Magnétisme non colinéaire, Composé intermétallique, Réseau hexagonal, Thulium alliage, Argent alliage, Silicium alliage, Lanthanide alliage.
English descriptors
- KwdEn :
- Antiferromagnetism, Canted spin arrangements, Crystal structure, Ferromagnetism, Hexagonal lattices, Intermetallic compounds, Magnetic moments, Magnetic structure, Neutron diffraction, Noncollinear magnetism, RKKY interaction, Rare earth alloys, Silicon alloys, Silver alloys, Specific heat, Thulium alloys.
Abstract
The ternary intermetallic TmAgSi compound which crystallizes in the hexagonal ZrNiAl-type crystal structure. TmAgSi has been investigated by means of magnetic, heat capacity and neutron diffraction measurements. The experimental data revealed the presence of an antiferromagnetic ordering below TN = 3.3 K with the magnetic moments lying within the basal plane. At 1.5 K they are equal to 6.31 (6) μB. The determined magnetic structure is non-collinear and can be described by three different propagation vectors: k? = [1/2,0,0], k?'= [-1/2,1/2,0] and k?"= [0,-1/2,0].
| pA |
|
|---|
Links toward previous steps (curation, corpus...)
- to stream Pascal, to step Corpus: Pour aller vers cette notice dans l'étape Curation :000299
Links to Exploration step
Pascal:10-0505124Le document en format XML
<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Magnetic behavior in TmAgSi</title><author><name sortKey="Baran, S" sort="Baran, S" uniqKey="Baran S" first="S." last="Baran">S. Baran</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Kaczorowski, D" sort="Kaczorowski, D" uniqKey="Kaczorowski D" first="D." last="Kaczorowski">D. Kaczorowski</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410</s1><s2>50 950 Wroclaw</s2><s3>POL</s3><sZ>2 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Hoser, A" sort="Hoser, A" uniqKey="Hoser A" first="A." last="Hoser">A. Hoser</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Helmholtz-Zentrum Berlin, Glienicker Str. 100</s1><s2>14 109 Berlin</s2><s3>DEU</s3><sZ>3 aut.</sZ></inist:fA14><country>Allemagne</country></affiliation></author><author><name sortKey="Penc, B" sort="Penc, B" uniqKey="Penc B" first="B." last="Penc">B. Penc</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Szytula, A" sort="Szytula, A" uniqKey="Szytula A" first="A." last="Szytula">A. Szytula</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">INIST</idno><idno type="inist">10-0505124</idno><date when="2011">2011</date><idno type="stanalyst">PASCAL 10-0505124 INIST</idno><idno type="RBID">Pascal:10-0505124</idno><idno type="wicri:Area/Pascal/Corpus">000299</idno><idno type="wicri:Area/Pascal/Curation">000299</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetic behavior in TmAgSi</title><author><name sortKey="Baran, S" sort="Baran, S" uniqKey="Baran S" first="S." last="Baran">S. Baran</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Kaczorowski, D" sort="Kaczorowski, D" uniqKey="Kaczorowski D" first="D." last="Kaczorowski">D. Kaczorowski</name><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410</s1><s2>50 950 Wroclaw</s2><s3>POL</s3><sZ>2 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Hoser, A" sort="Hoser, A" uniqKey="Hoser A" first="A." last="Hoser">A. Hoser</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Helmholtz-Zentrum Berlin, Glienicker Str. 100</s1><s2>14 109 Berlin</s2><s3>DEU</s3><sZ>3 aut.</sZ></inist:fA14><country>Allemagne</country></affiliation></author><author><name sortKey="Penc, B" sort="Penc, B" uniqKey="Penc B" first="B." last="Penc">B. Penc</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author><author><name sortKey="Szytula, A" sort="Szytula, A" uniqKey="Szytula A" first="A." last="Szytula">A. Szytula</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Pologne</country></affiliation></author></analytic><series><title level="j" type="main">Journal of magnetism and magnetic materials</title><title level="j" type="abbreviated">J. magn. magn. mater.</title><idno type="ISSN">0304-8853</idno><imprint><date when="2011">2011</date></imprint></series></biblStruct></sourceDesc><seriesStmt><title level="j" type="main">Journal of magnetism and magnetic materials</title><title level="j" type="abbreviated">J. magn. magn. mater.</title><idno type="ISSN">0304-8853</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Antiferromagnetism</term><term>Canted spin arrangements</term><term>Crystal structure</term><term>Ferromagnetism</term><term>Hexagonal lattices</term><term>Intermetallic compounds</term><term>Magnetic moments</term><term>Magnetic structure</term><term>Neutron diffraction</term><term>Noncollinear magnetism</term><term>RKKY interaction</term><term>Rare earth alloys</term><term>Silicon alloys</term><term>Silver alloys</term><term>Specific heat</term><term>Thulium alloys</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Structure cristalline</term><term>Chaleur massique</term><term>Diffraction neutron</term><term>Antiferromagnétisme</term><term>Moment magnétique</term><term>Structure magnétique</term><term>Ferromagnétisme</term><term>Structure spin incliné</term><term>Interaction RKKY</term><term>Magnétisme non colinéaire</term><term>Composé intermétallique</term><term>Réseau hexagonal</term><term>Thulium alliage</term><term>Argent alliage</term><term>Silicium alliage</term><term>Lanthanide alliage</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">The ternary intermetallic TmAgSi compound which crystallizes in the hexagonal ZrNiAl-type crystal structure. TmAgSi has been investigated by means of magnetic, heat capacity and neutron diffraction measurements. The experimental data revealed the presence of an antiferromagnetic ordering below T<sub>N</sub> <sub>=</sub> 3.3 K with the magnetic moments lying within the basal plane. At 1.5 K they are equal to 6.31 (6) μ<sub>B</sub>. The determined magnetic structure is non-collinear and can be described by three different propagation vectors: k? = [1/2,0,0], k?'= [-1/2,1/2,0] and k?"= [0,-1/2,0].</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0304-8853</s0></fA01><fA02 i1="01"><s0>JMMMDC</s0></fA02><fA03 i2="1"><s0>J. magn. magn. mater.</s0></fA03><fA05><s2>323</s2></fA05><fA06><s2>2</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Magnetic behavior in TmAgSi</s1></fA08><fA11 i1="01" i2="1"><s1>BARAN (S.)</s1></fA11><fA11 i1="02" i2="1"><s1>KACZOROWSKI (D.)</s1></fA11><fA11 i1="03" i2="1"><s1>HOSER (A.)</s1></fA11><fA11 i1="04" i2="1"><s1>PENC (B.)</s1></fA11><fA11 i1="05" i2="1"><s1>SZYTULA (A.)</s1></fA11><fA14 i1="01"><s1>M. Smoluchowski Institute of Physics, Jagiellonian University, Reymonta 4</s1><s2>30 059 Kraków</s2><s3>POL</s3><sZ>1 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></fA14><fA14 i1="02"><s1>Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410</s1><s2>50 950 Wroclaw</s2><s3>POL</s3><sZ>2 aut.</sZ></fA14><fA14 i1="03"><s1>Helmholtz-Zentrum Berlin, Glienicker Str. 100</s1><s2>14 109 Berlin</s2><s3>DEU</s3><sZ>3 aut.</sZ></fA14><fA20><s1>222-225</s1></fA20><fA21><s1>2011</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>17230</s2><s5>354000193343180060</s5></fA43><fA44><s0>0000</s0><s1>© 2010 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>11 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>10-0505124</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of magnetism and magnetic materials</s0></fA64><fA66 i1="01"><s0>NLD</s0></fA66><fC01 i1="01" l="ENG"><s0>The ternary intermetallic TmAgSi compound which crystallizes in the hexagonal ZrNiAl-type crystal structure. TmAgSi has been investigated by means of magnetic, heat capacity and neutron diffraction measurements. The experimental data revealed the presence of an antiferromagnetic ordering below T<sub>N</sub> <sub>=</sub> 3.3 K with the magnetic moments lying within the basal plane. At 1.5 K they are equal to 6.31 (6) μ<sub>B</sub>. The determined magnetic structure is non-collinear and can be described by three different propagation vectors: k? = [1/2,0,0], k?'= [-1/2,1/2,0] and k?"= [0,-1/2,0].</s0></fC01><fC02 i1="01" i2="3"><s0>001B70E25</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Structure cristalline</s0><s5>02</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Crystal structure</s0><s5>02</s5></fC03><fC03 i1="02" i2="3" l="FRE"><s0>Chaleur massique</s0><s5>03</s5></fC03><fC03 i1="02" i2="3" l="ENG"><s0>Specific heat</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Diffraction neutron</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Neutron diffraction</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Antiferromagnétisme</s0><s5>05</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Antiferromagnetism</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Moment magnétique</s0><s5>06</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Magnetic moments</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Structure magnétique</s0><s5>07</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Magnetic structure</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Ferromagnétisme</s0><s5>08</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Ferromagnetism</s0><s5>08</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Structure spin incliné</s0><s5>09</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Canted spin arrangements</s0><s5>09</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Interaction RKKY</s0><s5>10</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>RKKY interaction</s0><s5>10</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Magnétisme non colinéaire</s0><s5>11</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Noncollinear magnetism</s0><s5>11</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Composé intermétallique</s0><s5>15</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Intermetallic compounds</s0><s5>15</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Réseau hexagonal</s0><s5>16</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Hexagonal lattices</s0><s5>16</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Thulium alliage</s0><s5>17</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Thulium alloys</s0><s5>17</s5></fC03><fC03 i1="14" i2="3" l="FRE"><s0>Argent alliage</s0><s5>18</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Silver alloys</s0><s5>18</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Silicium alliage</s0><s5>19</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>Silicon alloys</s0><s5>19</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Lanthanide alliage</s0><s5>48</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Rare earth alloys</s0><s5>48</s5></fC03><fN21><s1>341</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 000299 | SxmlIndent | more
Ou
HfdSelect -h $EXPLOR_AREA/Data/Pascal/Curation/biblio.hfd -nk 000299 | 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:10-0505124
|texte= Magnetic behavior in TmAgSi
}}
| This area was generated with Dilib version V0.6.21. |  |