Magnetic study of HfFe6Ge6-type solid solutions TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0)
Identifieur interne : 000E93 ( Pascal/Corpus ); précédent : 000E92; suivant : 000E94Magnetic study of HfFe6Ge6-type solid solutions TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0)
Auteurs : G. VenturiniSource :
- Journal of alloys and compounds [ 0925-8388 ] ; 2000.
Descripteurs français
- Pascal (Inist)
- Aimantation, Ordre magnétique, Ferrimagnétisme, Antiferromagnétisme, Dépendance température, Réorientation spin, Hystérésis magnétique, Interaction échange, Effet composition, Solution solide, Terbium alliage, Manganèse alliage, Germanium alliage, Gallium alliage, Thulium alliage, Alliage quaternaire, Etude expérimentale, Alliage GaGeMnTb, Ga Ge Mn Tb, Alliage GaGeMnTm, Ga Ge Mn Tm, 7525, 7560E.
English descriptors
- KwdEn :
- Antiferromagnetism, Composition effect, Exchange interactions, Experimental study, Ferrimagnetism, Gallium alloys, Germanium alloys, Magnetic hysteresis, Magnetic ordering, Magnetization, Manganese alloys, Quaternary alloys, Solid solutions, Spin reorientation, Temperature dependence, Terbium alloys, Thulium alloys.
Abstract
The TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0) compounds have been studied by magnetization measurements in the temperature range 10-600 K. The TbMn6Ge6-xGax compounds order ferrimagnetically above room temperature (452≥Tc≥438 K). The low Ga content compounds (x≤0.2) display a ferri- to antiferromagnetic transition on cooling (363≥T1≥181 K) and a second Curie point at lower temperature (49≤Ty≤108 K). The high Ga content compounds display ferrimagnetic ordering in their whole ordered range and a spin reorientation transition at low temperature (112≤TSF≤162 K). The TmMn6Ge6-xGax compounds (x≤0.8) order antiferromagnetically above the room temperature (476≥TN≥372 K) and except TmMn6Ge5-8Ga0.2, display a ferrimagnetic ordering at lower temperature (32≤Tc≤250 K). TmMn6GF5Ga is ferrimagnetic in its whole ordered range. The Ga-rich compounds (x≥0.6) display a spin reorientation process around 50 K. All the ferrimagnetic compounds display large anisotropy effects at low temperature. The coercive fields measured for TbMn6Ge5.4Ga0.6 and TmMn6Ge5Ga1 are greater than 25 and 20 kOe, respectively. The evolutions of the magnetic properties and magnetocrystalline anisotropy are discussed.
Notice en format standard (ISO 2709)
Pour connaître la documentation sur le format Inist Standard.
| pA |
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Format Inist (serveur)
| NO : | PASCAL 01-0056184 INIST |
|---|---|
| ET : | Magnetic study of HfFe6Ge6-type solid solutions TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0) |
| AU : | VENTURINI (G.) |
| AF : | Laboratoire de Chimie du Solide Minéral, Université Henri Poincaré-Nancy I, associé au CNRS (UMR 7555), B.P. 239/54506 Vandoeuvre les Nancy/France (1 aut.) |
| DT : | Publication en série; Niveau analytique |
| SO : | Journal of alloys and compounds; ISSN 0925-8388; Suisse; Da. 2000; Vol. 313; No. 1-2; Pp. 26-33; Bibl. 21 ref. |
| LA : | Anglais |
| EA : | The TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0) compounds have been studied by magnetization measurements in the temperature range 10-600 K. The TbMn6Ge6-xGa x compounds order ferrimagnetically above room temperature (452≥Tc≥438 K). The low Ga content compounds (x≤0.2) display a ferri- to antiferromagnetic transition on cooling (363≥T1≥181 K) and a second Curie point at lower temperature (49≤Ty≤108 K). The high Ga content compounds display ferrimagnetic ordering in their whole ordered range and a spin reorientation transition at low temperature (112≤TSF≤162 K). The TmMn6Ge6-xGax compounds (x≤0.8) order antiferromagnetically above the room temperature (476≥TN≥372 K) and except TmMn6Ge5-8Ga 0.2, display a ferrimagnetic ordering at lower temperature (32≤Tc≤250 K). TmMn6GF5Ga is ferrimagnetic in its whole ordered range. The Ga-rich compounds (x≥0.6) display a spin reorientation process around 50 K. All the ferrimagnetic compounds display large anisotropy effects at low temperature. The coercive fields measured for TbMn6Ge5.4Ga0.6 and TmMn6Ge5Ga1 are greater than 25 and 20 kOe, respectively. The evolutions of the magnetic properties and magnetocrystalline anisotropy are discussed. |
| CC : | 001B70E25; 001B70E60E; 240 |
| FD : | Aimantation; Ordre magnétique; Ferrimagnétisme; Antiferromagnétisme; Dépendance température; Réorientation spin; Hystérésis magnétique; Interaction échange; Effet composition; Solution solide; Terbium alliage; Manganèse alliage; Germanium alliage; Gallium alliage; Thulium alliage; Alliage quaternaire; Etude expérimentale; Alliage GaGeMnTb; Ga Ge Mn Tb; Alliage GaGeMnTm; Ga Ge Mn Tm; 7525; 7560E |
| FG : | Lanthanide alliage; Métal transition alliage |
| ED : | Magnetization; Magnetic ordering; Ferrimagnetism; Antiferromagnetism; Temperature dependence; Spin reorientation; Magnetic hysteresis; Exchange interactions; Composition effect; Solid solutions; Terbium alloys; Manganese alloys; Germanium alloys; Gallium alloys; Thulium alloys; Quaternary alloys; Experimental study |
| EG : | Rare earth alloys; Transition element alloys |
| GD : | Konzentrationseinfluss |
| SD : | Reorientación spin; Efecto composición |
| LO : | INIST-1151.354000093754380100 |
| ID : | 01-0056184 |
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Pascal:01-0056184Le document en format XML
<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Magnetic study of HfFe<sub>6</sub>Ge<sub>6</sub>-type solid solutions TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0)</title><author><name sortKey="Venturini, G" sort="Venturini, G" uniqKey="Venturini G" first="G." last="Venturini">G. Venturini</name><affiliation><inist:fA14 i1="01"><s1>Laboratoire de Chimie du Solide Minéral, Université Henri Poincaré-Nancy I, associé au CNRS (UMR 7555), B.P. 239</s1><s2>54506 Vandoeuvre les Nancy</s2><s3>FRA</s3><sZ>1 aut.</sZ></inist:fA14></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">INIST</idno><idno type="inist">01-0056184</idno><date when="2000">2000</date><idno type="stanalyst">PASCAL 01-0056184 INIST</idno><idno type="RBID">Pascal:01-0056184</idno><idno type="wicri:Area/Pascal/Corpus">000E93</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetic study of HfFe<sub>6</sub>Ge<sub>6</sub>-type solid solutions TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0)</title><author><name sortKey="Venturini, G" sort="Venturini, G" uniqKey="Venturini G" first="G." last="Venturini">G. Venturini</name><affiliation><inist:fA14 i1="01"><s1>Laboratoire de Chimie du Solide Minéral, Université Henri Poincaré-Nancy I, associé au CNRS (UMR 7555), B.P. 239</s1><s2>54506 Vandoeuvre les Nancy</s2><s3>FRA</s3><sZ>1 aut.</sZ></inist:fA14></affiliation></author></analytic><series><title level="j" type="main">Journal of alloys and compounds</title><title level="j" type="abbreviated">J. alloys compd.</title><idno type="ISSN">0925-8388</idno><imprint><date when="2000">2000</date></imprint></series></biblStruct></sourceDesc><seriesStmt><title level="j" type="main">Journal of alloys and compounds</title><title level="j" type="abbreviated">J. alloys compd.</title><idno type="ISSN">0925-8388</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Antiferromagnetism</term><term>Composition effect</term><term>Exchange interactions</term><term>Experimental study</term><term>Ferrimagnetism</term><term>Gallium alloys</term><term>Germanium alloys</term><term>Magnetic hysteresis</term><term>Magnetic ordering</term><term>Magnetization</term><term>Manganese alloys</term><term>Quaternary alloys</term><term>Solid solutions</term><term>Spin reorientation</term><term>Temperature dependence</term><term>Terbium alloys</term><term>Thulium alloys</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Aimantation</term><term>Ordre magnétique</term><term>Ferrimagnétisme</term><term>Antiferromagnétisme</term><term>Dépendance température</term><term>Réorientation spin</term><term>Hystérésis magnétique</term><term>Interaction échange</term><term>Effet composition</term><term>Solution solide</term><term>Terbium alliage</term><term>Manganèse alliage</term><term>Germanium alliage</term><term>Gallium alliage</term><term>Thulium alliage</term><term>Alliage quaternaire</term><term>Etude expérimentale</term><term>Alliage GaGeMnTb</term><term>Ga Ge Mn Tb</term><term>Alliage GaGeMnTm</term><term>Ga Ge Mn Tm</term><term>7525</term><term>7560E</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0) compounds have been studied by magnetization measurements in the temperature range 10-600 K. The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> compounds order ferrimagnetically above room temperature (452≥T<sub>c</sub>≥438 K). The low Ga content compounds (x≤0.2) display a ferri- to antiferromagnetic transition on cooling (363≥T<sub>1</sub>≥181 K) and a second Curie point at lower temperature (49≤T<sub>y</sub>≤108 K). The high Ga content compounds display ferrimagnetic ordering in their whole ordered range and a spin reorientation transition at low temperature (112≤T<sub>SF</sub>≤162 K). The TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> compounds (x≤0.8) order antiferromagnetically above the room temperature (476≥TN≥372 K) and except TmMn<sub>6</sub>Ge<sub>5-8</sub>Ga<sub>0.2</sub>, display a ferrimagnetic ordering at lower temperature (32≤T<sub>c</sub>≤250 K). TmMn<sub>6</sub>GF<sub>5</sub>Ga is ferrimagnetic in its whole ordered range. The Ga-rich compounds (x≥0.6) display a spin reorientation process around 50 K. All the ferrimagnetic compounds display large anisotropy effects at low temperature. The coercive fields measured for TbMn<sub>6</sub>Ge<sub>5.</sub>4Ga<sub>0.6</sub> and TmMn<sub>6</sub>Ge<sub>5</sub>Ga<sub>1</sub> are greater than 25 and 20 kOe, respectively. The evolutions of the magnetic properties and magnetocrystalline anisotropy are discussed.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0925-8388</s0></fA01><fA03 i2="1"><s0>J. alloys compd.</s0></fA03><fA05><s2>313</s2></fA05><fA06><s2>1-2</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Magnetic study of HfFe<sub>6</sub>Ge<sub>6</sub>-type solid solutions TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0)</s1></fA08><fA11 i1="01" i2="1"><s1>VENTURINI (G.)</s1></fA11><fA14 i1="01"><s1>Laboratoire de Chimie du Solide Minéral, Université Henri Poincaré-Nancy I, associé au CNRS (UMR 7555), B.P. 239</s1><s2>54506 Vandoeuvre les Nancy</s2><s3>FRA</s3><sZ>1 aut.</sZ></fA14><fA20><s1>26-33</s1></fA20><fA21><s1>2000</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>1151</s2><s5>354000093754380100</s5></fA43><fA44><s0>0000</s0><s1>© 2001 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>21 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>01-0056184</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of alloys and compounds</s0></fA64><fA66 i1="01"><s0>CHE</s0></fA66><fC01 i1="01" l="ENG"><s0>The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0) compounds have been studied by magnetization measurements in the temperature range 10-600 K. The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> compounds order ferrimagnetically above room temperature (452≥T<sub>c</sub>≥438 K). The low Ga content compounds (x≤0.2) display a ferri- to antiferromagnetic transition on cooling (363≥T<sub>1</sub>≥181 K) and a second Curie point at lower temperature (49≤T<sub>y</sub>≤108 K). The high Ga content compounds display ferrimagnetic ordering in their whole ordered range and a spin reorientation transition at low temperature (112≤T<sub>SF</sub>≤162 K). The TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> compounds (x≤0.8) order antiferromagnetically above the room temperature (476≥TN≥372 K) and except TmMn<sub>6</sub>Ge<sub>5-8</sub>Ga<sub>0.2</sub>, display a ferrimagnetic ordering at lower temperature (32≤T<sub>c</sub>≤250 K). TmMn<sub>6</sub>GF<sub>5</sub>Ga is ferrimagnetic in its whole ordered range. The Ga-rich compounds (x≥0.6) display a spin reorientation process around 50 K. All the ferrimagnetic compounds display large anisotropy effects at low temperature. The coercive fields measured for TbMn<sub>6</sub>Ge<sub>5.</sub>4Ga<sub>0.6</sub> and TmMn<sub>6</sub>Ge<sub>5</sub>Ga<sub>1</sub> are greater than 25 and 20 kOe, respectively. The evolutions of the magnetic properties and magnetocrystalline anisotropy are discussed.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70E25</s0></fC02><fC02 i1="02" i2="3"><s0>001B70E60E</s0></fC02><fC02 i1="03" i2="X"><s0>240</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Aimantation</s0><s5>01</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Magnetization</s0><s5>01</s5></fC03><fC03 i1="02" i2="3" l="FRE"><s0>Ordre magnétique</s0><s5>02</s5></fC03><fC03 i1="02" i2="3" l="ENG"><s0>Magnetic ordering</s0><s5>02</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Ferrimagnétisme</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Ferrimagnetism</s0><s5>03</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Antiferromagnétisme</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Antiferromagnetism</s0><s5>04</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Dépendance température</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Temperature dependence</s0><s5>05</s5></fC03><fC03 i1="06" i2="X" l="FRE"><s0>Réorientation spin</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="ENG"><s0>Spin reorientation</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="SPA"><s0>Reorientación spin</s0><s5>06</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Hystérésis magnétique</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Magnetic hysteresis</s0><s5>07</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Interaction échange</s0><s5>09</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Exchange interactions</s0><s5>09</s5></fC03><fC03 i1="09" i2="X" l="FRE"><s0>Effet composition</s0><s5>10</s5></fC03><fC03 i1="09" i2="X" l="ENG"><s0>Composition effect</s0><s5>10</s5></fC03><fC03 i1="09" i2="X" l="GER"><s0>Konzentrationseinfluss</s0><s5>10</s5></fC03><fC03 i1="09" i2="X" l="SPA"><s0>Efecto composición</s0><s5>10</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Solution solide</s0><s5>11</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Solid solutions</s0><s5>11</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Terbium alliage</s0><s5>12</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Terbium alloys</s0><s5>12</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Manganèse alliage</s0><s5>13</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Manganese alloys</s0><s5>13</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Germanium alliage</s0><s5>14</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Germanium alloys</s0><s5>14</s5></fC03><fC03 i1="14" i2="3" l="FRE"><s0>Gallium alliage</s0><s5>15</s5></fC03><fC03 i1="14" i2="3" l="ENG"><s0>Gallium alloys</s0><s5>15</s5></fC03><fC03 i1="15" i2="3" l="FRE"><s0>Thulium alliage</s0><s5>16</s5></fC03><fC03 i1="15" i2="3" l="ENG"><s0>Thulium alloys</s0><s5>16</s5></fC03><fC03 i1="16" i2="3" l="FRE"><s0>Alliage quaternaire</s0><s5>17</s5></fC03><fC03 i1="16" i2="3" l="ENG"><s0>Quaternary alloys</s0><s5>17</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Etude expérimentale</s0><s5>18</s5></fC03><fC03 i1="17" i2="3" l="ENG"><s0>Experimental study</s0><s5>18</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>Alliage GaGeMnTb</s0><s2>NK</s2><s4>INC</s4><s5>52</s5></fC03><fC03 i1="19" i2="3" l="FRE"><s0>Ga Ge Mn Tb</s0><s4>INC</s4><s5>53</s5></fC03><fC03 i1="20" i2="3" l="FRE"><s0>Alliage GaGeMnTm</s0><s2>NK</s2><s4>INC</s4><s5>54</s5></fC03><fC03 i1="21" i2="3" l="FRE"><s0>Ga Ge Mn Tm</s0><s4>INC</s4><s5>55</s5></fC03><fC03 i1="22" i2="3" l="FRE"><s0>7525</s0><s2>PAC</s2><s4>INC</s4><s5>56</s5></fC03><fC03 i1="23" i2="3" l="FRE"><s0>7560E</s0><s2>PAC</s2><s4>INC</s4><s5>57</s5></fC03><fC07 i1="01" i2="3" l="FRE"><s0>Lanthanide alliage</s0><s5>48</s5></fC07><fC07 i1="01" i2="3" l="ENG"><s0>Rare earth alloys</s0><s5>48</s5></fC07><fC07 i1="02" i2="3" l="FRE"><s0>Métal transition alliage</s0><s5>49</s5></fC07><fC07 i1="02" i2="3" l="ENG"><s0>Transition element alloys</s0><s5>49</s5></fC07><fN21><s1>036</s1></fN21></pA></standard><server><NO>PASCAL 01-0056184 INIST</NO><ET>Magnetic study of HfFe<sub>6</sub>Ge<sub>6</sub>-type solid solutions TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0)</ET><AU>VENTURINI (G.)</AU><AF>Laboratoire de Chimie du Solide Minéral, Université Henri Poincaré-Nancy I, associé au CNRS (UMR 7555), B.P. 239/54506 Vandoeuvre les Nancy/France (1 aut.)</AF><DT>Publication en série; Niveau analytique</DT><SO>Journal of alloys and compounds; ISSN 0925-8388; Suisse; Da. 2000; Vol. 313; No. 1-2; Pp. 26-33; Bibl. 21 ref.</SO><LA>Anglais</LA><EA>The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.05≤x≤0.60) and TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> (0.2≤x≤1.0) compounds have been studied by magnetization measurements in the temperature range 10-600 K. The TbMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub> x</sub> compounds order ferrimagnetically above room temperature (452≥T<sub>c</sub>≥438 K). The low Ga content compounds (x≤0.2) display a ferri- to antiferromagnetic transition on cooling (363≥T<sub>1</sub>≥181 K) and a second Curie point at lower temperature (49≤T<sub>y</sub>≤108 K). The high Ga content compounds display ferrimagnetic ordering in their whole ordered range and a spin reorientation transition at low temperature (112≤T<sub>SF</sub>≤162 K). The TmMn<sub>6</sub>Ge<sub>6-x</sub>Ga<sub>x</sub> compounds (x≤0.8) order antiferromagnetically above the room temperature (476≥TN≥372 K) and except TmMn<sub>6</sub>Ge<sub>5-8</sub>Ga<sub> 0.2</sub>, display a ferrimagnetic ordering at lower temperature (32≤T<sub>c</sub>≤250 K). TmMn<sub>6</sub>GF<sub>5</sub>Ga is ferrimagnetic in its whole ordered range. The Ga-rich compounds (x≥0.6) display a spin reorientation process around 50 K. All the ferrimagnetic compounds display large anisotropy effects at low temperature. The coercive fields measured for TbMn<sub>6</sub>Ge<sub>5.</sub>4Ga<sub>0.6</sub> and TmMn<sub>6</sub>Ge<sub>5</sub>Ga<sub>1</sub> are greater than 25 and 20 kOe, respectively. The evolutions of the magnetic properties and magnetocrystalline anisotropy are discussed.</EA><CC>001B70E25; 001B70E60E; 240</CC><FD>Aimantation; Ordre magnétique; Ferrimagnétisme; Antiferromagnétisme; Dépendance température; Réorientation spin; Hystérésis magnétique; Interaction échange; Effet composition; Solution solide; Terbium alliage; Manganèse alliage; Germanium alliage; Gallium alliage; Thulium alliage; Alliage quaternaire; Etude expérimentale; Alliage GaGeMnTb; Ga Ge Mn Tb; Alliage GaGeMnTm; Ga Ge Mn Tm; 7525; 7560E</FD><FG>Lanthanide alliage; Métal transition alliage</FG><ED>Magnetization; Magnetic ordering; Ferrimagnetism; Antiferromagnetism; Temperature dependence; Spin reorientation; Magnetic hysteresis; Exchange interactions; Composition effect; Solid solutions; Terbium alloys; Manganese alloys; Germanium alloys; Gallium alloys; Thulium alloys; Quaternary alloys; Experimental study</ED><EG>Rare earth alloys; Transition element alloys</EG><GD>Konzentrationseinfluss</GD><SD>Reorientación spin; Efecto composición</SD><LO>INIST-1151.354000093754380100</LO><ID>01-0056184</ID></server></inist></record>Pour manipuler ce document sous Unix (Dilib)
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|étape= Corpus
|type= RBID
|clé= Pascal:01-0056184
|texte= Magnetic study of HfFe6Ge6-type solid solutions TbMn6Ge6-xGax (0.05≤x≤0.60) and TmMn6Ge6-xGax (0.2≤x≤1.0)
}}
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