Magnetic properties of the RNi4Mn (R = Gd, Tb, Dy, Ho, Er, Tm, and Y) intermetallics
Identifieur interne :
000E30 ( Pascal/Curation );
précédent :
000E29;
suivant :
000E31
Magnetic properties of the RNi4Mn (R = Gd, Tb, Dy, Ho, Er, Tm, and Y) intermetallics
Auteurs : I. S. Dubenko [
États-Unis,
Russie] ;
I. Yu. Gaidukova [
Russie] ;
S. A. Granovsky [
Russie] ;
V. Rodimin [
Russie] ;
A. S. Markosyan [
Russie] ;
S. Roy [
États-Unis] ;
N. Ali [
États-Unis]
Source :
-
IEEE transactions on magnetics [ 0018-9464 ] ; 2000.
RBID : Pascal:01-0234339
Descripteurs français
- Pascal (Inist)
- Propriété magnétique,
Alliage base nickel,
Manganèse alliage,
Yttrium alliage,
Composé intermétallique,
Alliage ternaire,
Transition phase,
Gadolinium alliage,
Terbium alliage,
Dysprosium alliage,
Thulium alliage,
Lanthanide alliage,
Diffraction RX,
Caractéristique magnétique,
Dépendance température,
Etude expérimentale,
Holmium alliage,
Erbium alliage,
7550W.
English descriptors
- KwdEn :
- Dysprosium alloys,
Erbium alloys,
Experimental study,
Gadolinium alloys,
Holmium alloys,
Intermetallic compounds,
Magnetic properties,
Magnetization curve,
Manganese alloys,
Nickel base alloys,
Phase transitions,
Rare earth alloys,
Temperature dependence,
Terbium alloys,
Ternary alloys,
Thulium alloys,
XRD,
Yttrium alloys.
Abstract
The magnetization of the RNi4Mn compounds (R = Gd-Tm and Y) was studied up to 55 kOe at 2K, and up to 400K at 30 kOe. A substantial increase of TCwith respect to nonsubstituted RNi5 series was found. The nonlinear variation of TC vs. R and the change of the high filed magnetization values is attributed to the Mn substitution. Field induced magnetic phase transitions were observed at 2K for R = Er and Tm. These transitions are suggested to occur due to the magnetic anisotropy in the rare earth sublattice.
| pA |
| A01 | 01 | 1 | | @0 0018-9464 |
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| A02 | 01 | | | @0 IEMGAQ |
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| A03 | | 1 | | @0 IEEE trans. magn. |
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| A05 | | | | @2 36 |
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| A06 | | | | @2 5 @3 PART1 |
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| A08 | 01 | 1 | ENG | @1 Magnetic properties of the RNi4Mn (R = Gd, Tb, Dy, Ho, Er, Tm, and Y) intermetallics |
|---|
| A09 | 01 | 1 | ENG | @1 Selected papers from the 2000 International Magnetics Conference (INTERMAG 2000), Toronto, Ontario, Canada, April 9-12, 2000 |
|---|
| A11 | 01 | 1 | | @1 DUBENKO (I. S.) |
|---|
| A11 | 02 | 1 | | @1 GAIDUKOVA (I. Yu.) |
|---|
| A11 | 03 | 1 | | @1 GRANOVSKY (S. A.) |
|---|
| A11 | 04 | 1 | | @1 RODIMIN (V.) |
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| A11 | 05 | 1 | | @1 MARKOSYAN (A. S.) |
|---|
| A11 | 06 | 1 | | @1 ROY (S.) |
|---|
| A11 | 07 | 1 | | @1 ALI (N.) |
|---|
| A14 | 01 | | | @1 Department of Physics, Southern Illinois University at Carbondale @2 Carbondale, IL 62901 @3 USA @Z 1 aut. @Z 6 aut. @Z 7 aut. |
|---|
| A14 | 02 | | | @1 Moscow Institute of Radio Engineering Electronics and Automation @2 117454 Moscow @3 RUS @Z 1 aut. |
|---|
| A14 | 03 | | | @1 Faculty of Physics, M. V. Lomonosov Moscow State University @2 119899 Moscow @3 RUS @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. |
|---|
| A18 | 01 | 1 | | @1 IEEE @3 INT @9 patr. |
|---|
| A20 | | | | @1 3336-3338 |
|---|
| A21 | | | | @1 2000 |
|---|
| A23 | 01 | | | @0 ENG |
|---|
| A43 | 01 | | | @1 INIST @2 222H6 @5 354000098009633560 |
|---|
| A44 | | | | @0 0000 @1 © 2001 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 7 ref. |
|---|
| A47 | 01 | 1 | | @0 01-0234339 |
|---|
| A60 | | | | @1 P @2 C |
|---|
| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 IEEE transactions on magnetics |
|---|
| A66 | 01 | | | @0 USA |
|---|
| C01 | 01 | | ENG | @0 The magnetization of the RNi4Mn compounds (R = Gd-Tm and Y) was studied up to 55 kOe at 2K, and up to 400K at 30 kOe. A substantial increase of TCwith respect to nonsubstituted RNi5 series was found. The nonlinear variation of TC vs. R and the change of the high filed magnetization values is attributed to the Mn substitution. Field induced magnetic phase transitions were observed at 2K for R = Er and Tm. These transitions are suggested to occur due to the magnetic anisotropy in the rare earth sublattice. |
|---|
| C02 | 01 | 3 | | @0 001B70E50W |
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| C02 | 02 | X | | @0 240 |
|---|
| C03 | 01 | 3 | FRE | @0 Propriété magnétique @5 01 |
|---|
| C03 | 01 | 3 | ENG | @0 Magnetic properties @5 01 |
|---|
| C03 | 02 | 3 | FRE | @0 Alliage base nickel @2 NK @5 02 |
|---|
| C03 | 02 | 3 | ENG | @0 Nickel base alloys @2 NK @5 02 |
|---|
| C03 | 03 | 3 | FRE | @0 Manganèse alliage @5 03 |
|---|
| C03 | 03 | 3 | ENG | @0 Manganese alloys @5 03 |
|---|
| C03 | 04 | 3 | FRE | @0 Yttrium alliage @5 04 |
|---|
| C03 | 04 | 3 | ENG | @0 Yttrium alloys @5 04 |
|---|
| C03 | 05 | 3 | FRE | @0 Composé intermétallique @5 05 |
|---|
| C03 | 05 | 3 | ENG | @0 Intermetallic compounds @5 05 |
|---|
| C03 | 06 | 3 | FRE | @0 Alliage ternaire @5 06 |
|---|
| C03 | 06 | 3 | ENG | @0 Ternary alloys @5 06 |
|---|
| C03 | 07 | X | FRE | @0 Transition phase @5 07 |
|---|
| C03 | 07 | X | ENG | @0 Phase transitions @5 07 |
|---|
| C03 | 07 | X | SPA | @0 Transición fase @5 07 |
|---|
| C03 | 08 | 3 | FRE | @0 Gadolinium alliage @5 08 |
|---|
| C03 | 08 | 3 | ENG | @0 Gadolinium alloys @5 08 |
|---|
| C03 | 09 | 3 | FRE | @0 Terbium alliage @5 09 |
|---|
| C03 | 09 | 3 | ENG | @0 Terbium alloys @5 09 |
|---|
| C03 | 10 | 3 | FRE | @0 Dysprosium alliage @5 10 |
|---|
| C03 | 10 | 3 | ENG | @0 Dysprosium alloys @5 10 |
|---|
| C03 | 11 | 3 | FRE | @0 Thulium alliage @5 11 |
|---|
| C03 | 11 | 3 | ENG | @0 Thulium alloys @5 11 |
|---|
| C03 | 12 | 3 | FRE | @0 Lanthanide alliage @5 12 |
|---|
| C03 | 12 | 3 | ENG | @0 Rare earth alloys @5 12 |
|---|
| C03 | 13 | 3 | FRE | @0 Diffraction RX @5 13 |
|---|
| C03 | 13 | 3 | ENG | @0 XRD @5 13 |
|---|
| C03 | 14 | X | FRE | @0 Caractéristique magnétique @5 14 |
|---|
| C03 | 14 | X | ENG | @0 Magnetization curve @5 14 |
|---|
| C03 | 14 | X | GER | @0 Magnetisierungskurve @5 14 |
|---|
| C03 | 14 | X | SPA | @0 Característica magnética @5 14 |
|---|
| C03 | 15 | 3 | FRE | @0 Dépendance température @5 15 |
|---|
| C03 | 15 | 3 | ENG | @0 Temperature dependence @5 15 |
|---|
| C03 | 16 | 3 | FRE | @0 Etude expérimentale @5 16 |
|---|
| C03 | 16 | 3 | ENG | @0 Experimental study @5 16 |
|---|
| C03 | 17 | 3 | FRE | @0 Holmium alliage @5 23 |
|---|
| C03 | 17 | 3 | ENG | @0 Holmium alloys @5 23 |
|---|
| C03 | 18 | 3 | FRE | @0 Erbium alliage @5 24 |
|---|
| C03 | 18 | 3 | ENG | @0 Erbium alloys @5 24 |
|---|
| C03 | 19 | 3 | FRE | @0 7550W @2 PAC @4 INC @5 95 |
|---|
| N21 | | | | @1 162 |
|---|
|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 Annual IEEE International Magnetics Conference (INTERMAG) @2 37 @3 Toronto, ON CAN @4 2000-04-09 |
|---|
|
|---|
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Le document en format XML
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</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Ali, N" sort="Ali, N" uniqKey="Ali N" first="N." last="Ali">N. Ali</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Southern Illinois University at Carbondale</s1>
<s2>Carbondale, IL 62901</s2>
<s3>USA</s3>
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<idno type="RBID">Pascal:01-0234339</idno>
<idno type="wicri:Area/Pascal/Corpus">000E30</idno>
<idno type="wicri:Area/Pascal/Curation">000E30</idno>
</publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Magnetic properties of the RNi<sub>4</sub>
Mn (R = Gd, Tb, Dy, Ho, Er, Tm, and Y) intermetallics</title><author><name sortKey="Dubenko, I S" sort="Dubenko, I S" uniqKey="Dubenko I" first="I. S." last="Dubenko">I. S. Dubenko</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Southern Illinois University at Carbondale</s1>
<s2>Carbondale, IL 62901</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Moscow Institute of Radio Engineering Electronics and Automation</s1>
<s2>117454 Moscow</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
</inist:fA14><country>Russie</country>
</affiliation><author><name sortKey="Gaidukova, I Yu" sort="Gaidukova, I Yu" uniqKey="Gaidukova I" first="I. Yu." last="Gaidukova">I. Yu. Gaidukova</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Faculty of Physics, M. V. Lomonosov Moscow State University</s1>
<s2>119899 Moscow</s2>
<s3>RUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>Russie</country>
</affiliation><author><name sortKey="Granovsky, S A" sort="Granovsky, S A" uniqKey="Granovsky S" first="S. A." last="Granovsky">S. A. Granovsky</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Faculty of Physics, M. V. Lomonosov Moscow State University</s1>
<s2>119899 Moscow</s2>
<s3>RUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>Russie</country>
</affiliation><author><name sortKey="Rodimin, V" sort="Rodimin, V" uniqKey="Rodimin V" first="V." last="Rodimin">V. Rodimin</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Faculty of Physics, M. V. Lomonosov Moscow State University</s1>
<s2>119899 Moscow</s2>
<s3>RUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>Russie</country>
</affiliation><author><name sortKey="Markosyan, A S" sort="Markosyan, A S" uniqKey="Markosyan A" first="A. S." last="Markosyan">A. S. Markosyan</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Faculty of Physics, M. V. Lomonosov Moscow State University</s1>
<s2>119899 Moscow</s2>
<s3>RUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>Russie</country>
</affiliation><author><name sortKey="Roy, S" sort="Roy, S" uniqKey="Roy S" first="S." last="Roy">S. Roy</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Southern Illinois University at Carbondale</s1>
<s2>Carbondale, IL 62901</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Ali, N" sort="Ali, N" uniqKey="Ali N" first="N." last="Ali">N. Ali</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Southern Illinois University at Carbondale</s1>
<s2>Carbondale, IL 62901</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><series><title level="j" type="main">IEEE transactions on magnetics</title>
<title level="j" type="abbreviated">IEEE trans. magn.</title>
<idno type="ISSN">0018-9464</idno>
<imprint><date when="2000">2000</date>
</imprint><seriesStmt><title level="j" type="main">IEEE transactions on magnetics</title>
<title level="j" type="abbreviated">IEEE trans. magn.</title>
<idno type="ISSN">0018-9464</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Dysprosium alloys</term>
<term>Erbium alloys</term>
<term>Experimental study</term>
<term>Gadolinium alloys</term>
<term>Holmium alloys</term>
<term>Intermetallic compounds</term>
<term>Magnetic properties</term>
<term>Magnetization curve</term>
<term>Manganese alloys</term>
<term>Nickel base alloys</term>
<term>Phase transitions</term>
<term>Rare earth alloys</term>
<term>Temperature dependence</term>
<term>Terbium alloys</term>
<term>Ternary alloys</term>
<term>Thulium alloys</term>
<term>XRD</term>
<term>Yttrium alloys</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Propriété magnétique</term>
<term>Alliage base nickel</term>
<term>Manganèse alliage</term>
<term>Yttrium alliage</term>
<term>Composé intermétallique</term>
<term>Alliage ternaire</term>
<term>Transition phase</term>
<term>Gadolinium alliage</term>
<term>Terbium alliage</term>
<term>Dysprosium alliage</term>
<term>Thulium alliage</term>
<term>Lanthanide alliage</term>
<term>Diffraction RX</term>
<term>Caractéristique magnétique</term>
<term>Dépendance température</term>
<term>Etude expérimentale</term>
<term>Holmium alliage</term>
<term>Erbium alliage</term>
<term>7550W</term>
</keywords><front><div type="abstract" xml:lang="en">The magnetization of the RNi<sub>4</sub>
Mn compounds (R = Gd-Tm and Y) was studied up to 55 kOe at 2K, and up to 400K at 30 kOe. A substantial increase of T<sub>C</sub>
with respect to nonsubstituted RNi<sub>5</sub>
series was found. The nonlinear variation of T<sub>C</sub>
vs. R and the change of the high filed magnetization values is attributed to the Mn substitution. Field induced magnetic phase transitions were observed at 2K for R = Er and Tm. These transitions are suggested to occur due to the magnetic anisotropy in the rare earth sublattice.</div><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0018-9464</s0>
</fA01><fA02 i1="01"><s0>IEMGAQ</s0>
</fA02><fA03 i2="1"><s0>IEEE trans. magn.</s0>
</fA03><fA06><s2>5</s2>
<s3>PART1</s3>
</fA06><fA08 i1="01" i2="1" l="ENG"><s1>Magnetic properties of the RNi<sub>4</sub>
Mn (R = Gd, Tb, Dy, Ho, Er, Tm, and Y) intermetallics</s1><fA09 i1="01" i2="1" l="ENG"><s1>Selected papers from the 2000 International Magnetics Conference (INTERMAG 2000), Toronto, Ontario, Canada, April 9-12, 2000</s1>
</fA09><fA11 i1="01" i2="1"><s1>DUBENKO (I. S.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>GAIDUKOVA (I. Yu.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>GRANOVSKY (S. A.)</s1>
</fA11><fA11 i1="04" i2="1"><s1>RODIMIN (V.)</s1>
</fA11><fA11 i1="05" i2="1"><s1>MARKOSYAN (A. S.)</s1>
</fA11><fA11 i1="06" i2="1"><s1>ROY (S.)</s1>
</fA11><fA11 i1="07" i2="1"><s1>ALI (N.)</s1>
</fA11><fA14 i1="01"><s1>Department of Physics, Southern Illinois University at Carbondale</s1>
<s2>Carbondale, IL 62901</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>7 aut.</sZ>
</fA14><fA14 i1="02"><s1>Moscow Institute of Radio Engineering Electronics and Automation</s1>
<s2>117454 Moscow</s2>
<s3>RUS</s3>
<sZ>1 aut.</sZ>
</fA14><fA14 i1="03"><s1>Faculty of Physics, M. V. Lomonosov Moscow State University</s1>
<s2>119899 Moscow</s2>
<s3>RUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14><fA18 i1="01" i2="1"><s1>IEEE</s1>
<s3>INT</s3>
<s9>patr.</s9>
</fA18><fA20><s1>3336-3338</s1>
</fA20><fA21><s1>2000</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA43 i1="01"><s1>INIST</s1>
<s2>222H6</s2>
<s5>354000098009633560</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2001 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>7 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>01-0234339</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>IEEE transactions on magnetics</s0>
</fA64><fA66 i1="01"><s0>USA</s0>
</fA66><fC01 i1="01" l="ENG"><s0>The magnetization of the RNi<sub>4</sub>
Mn compounds (R = Gd-Tm and Y) was studied up to 55 kOe at 2K, and up to 400K at 30 kOe. A substantial increase of T<sub>C</sub>
with respect to nonsubstituted RNi<sub>5</sub>
series was found. The nonlinear variation of T<sub>C</sub>
vs. R and the change of the high filed magnetization values is attributed to the Mn substitution. Field induced magnetic phase transitions were observed at 2K for R = Er and Tm. These transitions are suggested to occur due to the magnetic anisotropy in the rare earth sublattice.</s0><fC02 i1="01" i2="3"><s0>001B70E50W</s0>
</fC02><fC02 i1="02" i2="X"><s0>240</s0>
</fC02><fC03 i1="01" i2="3" l="FRE"><s0>Propriété magnétique</s0>
<s5>01</s5>
</fC03><fC03 i1="01" i2="3" l="ENG"><s0>Magnetic properties</s0>
<s5>01</s5>
</fC03><fC03 i1="02" i2="3" l="FRE"><s0>Alliage base nickel</s0>
<s2>NK</s2>
<s5>02</s5>
</fC03><fC03 i1="02" i2="3" l="ENG"><s0>Nickel base alloys</s0>
<s2>NK</s2>
<s5>02</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Manganèse alliage</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>Manganese alloys</s0>
<s5>03</s5>
</fC03><fC03 i1="04" i2="3" l="FRE"><s0>Yttrium alliage</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="3" l="ENG"><s0>Yttrium alloys</s0>
<s5>04</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Composé intermétallique</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Intermetallic compounds</s0>
<s5>05</s5>
</fC03><fC03 i1="06" i2="3" l="FRE"><s0>Alliage ternaire</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="3" l="ENG"><s0>Ternary alloys</s0>
<s5>06</s5>
</fC03><fC03 i1="07" i2="X" l="FRE"><s0>Transition phase</s0>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="ENG"><s0>Phase transitions</s0>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="SPA"><s0>Transición fase</s0>
<s5>07</s5>
</fC03><fC03 i1="08" i2="3" l="FRE"><s0>Gadolinium alliage</s0>
<s5>08</s5>
</fC03><fC03 i1="08" i2="3" l="ENG"><s0>Gadolinium alloys</s0>
<s5>08</s5>
</fC03><fC03 i1="09" i2="3" l="FRE"><s0>Terbium alliage</s0>
<s5>09</s5>
</fC03><fC03 i1="09" i2="3" l="ENG"><s0>Terbium alloys</s0>
<s5>09</s5>
</fC03><fC03 i1="10" i2="3" l="FRE"><s0>Dysprosium alliage</s0>
<s5>10</s5>
</fC03><fC03 i1="10" i2="3" l="ENG"><s0>Dysprosium alloys</s0>
<s5>10</s5>
</fC03><fC03 i1="11" i2="3" l="FRE"><s0>Thulium alliage</s0>
<s5>11</s5>
</fC03><fC03 i1="11" i2="3" l="ENG"><s0>Thulium alloys</s0>
<s5>11</s5>
</fC03><fC03 i1="12" i2="3" l="FRE"><s0>Lanthanide alliage</s0>
<s5>12</s5>
</fC03><fC03 i1="12" i2="3" l="ENG"><s0>Rare earth alloys</s0>
<s5>12</s5>
</fC03><fC03 i1="13" i2="3" l="FRE"><s0>Diffraction RX</s0>
<s5>13</s5>
</fC03><fC03 i1="13" i2="3" l="ENG"><s0>XRD</s0>
<s5>13</s5>
</fC03><fC03 i1="14" i2="X" l="FRE"><s0>Caractéristique magnétique</s0>
<s5>14</s5>
</fC03><fC03 i1="14" i2="X" l="ENG"><s0>Magnetization curve</s0>
<s5>14</s5>
</fC03><fC03 i1="14" i2="X" l="GER"><s0>Magnetisierungskurve</s0>
<s5>14</s5>
</fC03><fC03 i1="14" i2="X" l="SPA"><s0>Característica magnética</s0>
<s5>14</s5>
</fC03><fC03 i1="15" i2="3" l="FRE"><s0>Dépendance température</s0>
<s5>15</s5>
</fC03><fC03 i1="15" i2="3" l="ENG"><s0>Temperature dependence</s0>
<s5>15</s5>
</fC03><fC03 i1="16" i2="3" l="FRE"><s0>Etude expérimentale</s0>
<s5>16</s5>
</fC03><fC03 i1="16" i2="3" l="ENG"><s0>Experimental study</s0>
<s5>16</s5>
</fC03><fC03 i1="17" i2="3" l="FRE"><s0>Holmium alliage</s0>
<s5>23</s5>
</fC03><fC03 i1="17" i2="3" l="ENG"><s0>Holmium alloys</s0>
<s5>23</s5>
</fC03><fC03 i1="18" i2="3" l="FRE"><s0>Erbium alliage</s0>
<s5>24</s5>
</fC03><fC03 i1="18" i2="3" l="ENG"><s0>Erbium alloys</s0>
<s5>24</s5>
</fC03><fC03 i1="19" i2="3" l="FRE"><s0>7550W</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>95</s5>
</fC03><fN21><s1>162</s1>
</fN21><pR><fA30 i1="01" i2="1" l="ENG"><s1>Annual IEEE International Magnetics Conference (INTERMAG)</s1>
<s2>37</s2>
<s3>Toronto, ON CAN</s3>
<s4>2000-04-09</s4>
</fA30>
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