Pressure effect on the competition between ferromagnetic and antiferromagnetic spin fluctuations in TmTe investigated by 125Te-NMR
Identifieur interne :
000786 ( Pascal/Curation );
précédent :
000785;
suivant :
000787
Pressure effect on the competition between ferromagnetic and antiferromagnetic spin fluctuations in TmTe investigated by 125Te-NMR
Auteurs : A. Yamamoto [
Japon] ;
S. Wada [
Japon] ;
T. Matsumura [
Japon]
Source :
-
Journal of magnetism and magnetic materials [ 0304-8853 ] ; 2007.
RBID : Pascal:07-0194304
Descripteurs français
- Pascal (Inist)
- Effet pression,
Fluctuation spin,
Résonance magnétique nucléaire,
Relation ordre,
Valence intermédiaire,
Haute pression,
Ferromagnétisme,
Relaxation spin réseau,
Loi Curie Weiss,
Matériau ferromagnétique,
Thulium tellurure,
Semiconducteur magnétique,
TmTe,
7550P,
7660,
7530M.
English descriptors
- KwdEn :
- Curie-Weiss law,
Ferromagnetic materials,
Ferromagnetism,
High pressure,
Intermediate valence,
Magnetic semiconductors,
Nuclear magnetic resonance,
Ordering,
Pressure effects,
Spin fluctuations,
Spin-lattice relaxation,
Thulium tellurides.
Abstract
To elucidate from a microscopic point of view the initial evolution of spin fluctuations in TmTe from the semiconducting state at ambient pressure with an antiferroquadrupole ordering (TQ = 1.8K) to the intermediate-valence metallic state at high pressures P≥2 GPa with a ferromagnetic (FM) ordering (Tc ≃ 14 K), we have carried out 125Te-NMR study at pressures P = 0 and 0.9 GPa. The spin-lattice relaxation rate measurements revealed a pronounced increase of the staggered susceptibility below T≃ 14 K, in addition to the Curie-Weiss-type increase of the uniform susceptibility. Below ∼T*, a wipe-out decrease of the NMR intensity and the finding of an unconventional NMR signal around ∼ 10 MHz that is insensitive to applied field lead to the conclusion that a field-induced short-range FM ordering caused by the competition of FM and antiferromagnetic fluctuations takes place. Pressure of 0.9 GPa hardly affects the anomalous NMR behaviors below ∼T*, leading to speculate that the short-range FM ordering in the semiconducting state shares the origin with the long-range FM ordering at≃ 14K in the high-pressure metallic state.
pA |
A01 | 01 | 1 | | @0 0304-8853 |
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A02 | 01 | | | @0 JMMMDC |
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A03 | | 1 | | @0 J. magn. magn. mater. |
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A05 | | | | @2 310 |
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A06 | | | | @2 2 @3 p. 1 |
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A08 | 01 | 1 | ENG | @1 Pressure effect on the competition between ferromagnetic and antiferromagnetic spin fluctuations in TmTe investigated by 125Te-NMR |
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A09 | 01 | 1 | ENG | @1 Proceedings of the 17th International Conference on Magnetism (ICM 2006), Kyoto, 20-25 August 2006. Part I (Chapters 1-2) |
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A11 | 01 | 1 | | @1 YAMAMOTO (A.) |
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A11 | 02 | 1 | | @1 WADA (S.) |
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A11 | 03 | 1 | | @1 MATSUMURA (T.) |
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A12 | 01 | 1 | | @1 HARIMA (H.) @9 ed. |
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A12 | 02 | 1 | | @1 KAWAMURA (H.) @9 ed. |
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A12 | 03 | 1 | | @1 KITAOKA (Y.) @9 ed. |
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A12 | 04 | 1 | | @1 KOHNO (H.) @9 ed. |
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A12 | 05 | 1 | | @1 MIYAKE (K.) @9 ed. |
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A12 | 06 | 1 | | @1 SUZUKI (Y.) @9 ed. |
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A12 | 07 | 1 | | @1 SAKAKIMA (H.) @9 ed. |
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A12 | 08 | 1 | | @1 ZHENG (G.-q.) @9 ed. |
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A14 | 01 | | | @1 Department of Material Science, Graduate School of Science and Technology, Kobe University @2 Nada, Kobe 657-8501 @3 JPN @Z 1 aut. @Z 2 aut. |
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A14 | 02 | | | @1 Department of Physics, Graduate School of Science, Tohoku University @2 Sendai 980-8578 @3 JPN @Z 3 aut. |
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A15 | 01 | | | @1 Kobe University @3 JPN @Z 1 aut. |
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A15 | 02 | | | @1 Osaka University @3 JPN @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut. |
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A15 | 03 | | | @1 Matsushita Electric Industrial Co. Ltd. @3 JPN @Z 7 aut. |
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A15 | 04 | | | @1 Okayama University @3 JPN @Z 8 aut. |
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A18 | 01 | 1 | | @1 International Union for Pure and Applied Physics @3 INT @9 org-cong. |
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A20 | | | | @1 741-742 |
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A21 | | | | @1 2007 |
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A23 | 01 | | | @0 ENG |
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A43 | 01 | | | @1 INIST @2 17230 @5 354000159371061800 |
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A44 | | | | @0 0000 @1 © 2007 INIST-CNRS. All rights reserved. |
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A45 | | | | @0 8 ref. |
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A47 | 01 | 1 | | @0 07-0194304 |
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A60 | | | | @1 P @2 C |
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A61 | | | | @0 A |
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A64 | 01 | 1 | | @0 Journal of magnetism and magnetic materials |
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A66 | 01 | | | @0 NLD |
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C01 | 01 | | ENG | @0 To elucidate from a microscopic point of view the initial evolution of spin fluctuations in TmTe from the semiconducting state at ambient pressure with an antiferroquadrupole ordering (TQ = 1.8K) to the intermediate-valence metallic state at high pressures P≥2 GPa with a ferromagnetic (FM) ordering (Tc ≃ 14 K), we have carried out 125Te-NMR study at pressures P = 0 and 0.9 GPa. The spin-lattice relaxation rate measurements revealed a pronounced increase of the staggered susceptibility below T≃ 14 K, in addition to the Curie-Weiss-type increase of the uniform susceptibility. Below ∼T*, a wipe-out decrease of the NMR intensity and the finding of an unconventional NMR signal around ∼ 10 MHz that is insensitive to applied field lead to the conclusion that a field-induced short-range FM ordering caused by the competition of FM and antiferromagnetic fluctuations takes place. Pressure of 0.9 GPa hardly affects the anomalous NMR behaviors below ∼T*, leading to speculate that the short-range FM ordering in the semiconducting state shares the origin with the long-range FM ordering at≃ 14K in the high-pressure metallic state. |
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C02 | 01 | 3 | | @0 001B70E50P |
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C02 | 02 | 3 | | @0 001B70F60 |
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C02 | 03 | 3 | | @0 001B70E30M |
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C03 | 01 | 3 | FRE | @0 Effet pression @5 02 |
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C03 | 01 | 3 | ENG | @0 Pressure effects @5 02 |
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C03 | 02 | 3 | FRE | @0 Fluctuation spin @5 03 |
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C03 | 02 | 3 | ENG | @0 Spin fluctuations @5 03 |
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C03 | 03 | 3 | FRE | @0 Résonance magnétique nucléaire @5 04 |
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C03 | 03 | 3 | ENG | @0 Nuclear magnetic resonance @5 04 |
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C03 | 04 | X | FRE | @0 Relation ordre @5 05 |
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C03 | 04 | X | ENG | @0 Ordering @5 05 |
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C03 | 04 | X | SPA | @0 Relación orden @5 05 |
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C03 | 05 | 3 | FRE | @0 Valence intermédiaire @5 06 |
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C03 | 05 | 3 | ENG | @0 Intermediate valence @5 06 |
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C03 | 06 | 3 | FRE | @0 Haute pression @5 07 |
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C03 | 06 | 3 | ENG | @0 High pressure @5 07 |
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C03 | 07 | 3 | FRE | @0 Ferromagnétisme @5 08 |
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C03 | 07 | 3 | ENG | @0 Ferromagnetism @5 08 |
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C03 | 08 | 3 | FRE | @0 Relaxation spin réseau @5 09 |
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C03 | 08 | 3 | ENG | @0 Spin-lattice relaxation @5 09 |
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C03 | 09 | 3 | FRE | @0 Loi Curie Weiss @5 11 |
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C03 | 09 | 3 | ENG | @0 Curie-Weiss law @5 11 |
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C03 | 10 | 3 | FRE | @0 Matériau ferromagnétique @5 15 |
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C03 | 10 | 3 | ENG | @0 Ferromagnetic materials @5 15 |
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C03 | 11 | 3 | FRE | @0 Thulium tellurure @2 NK @5 16 |
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C03 | 11 | 3 | ENG | @0 Thulium tellurides @2 NK @5 16 |
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C03 | 12 | 3 | FRE | @0 Semiconducteur magnétique @5 18 |
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C03 | 12 | 3 | ENG | @0 Magnetic semiconductors @5 18 |
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C03 | 13 | 3 | FRE | @0 TmTe @4 INC @5 53 |
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C03 | 14 | 3 | FRE | @0 7550P @4 INC @5 60 |
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C03 | 15 | 3 | FRE | @0 7660 @4 INC @5 61 |
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C03 | 16 | 3 | FRE | @0 7530M @4 INC @5 62 |
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N21 | | | | @1 128 |
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|
pR |
A30 | 01 | 1 | ENG | @1 ICM 2006 : International Conference on Magnetism @2 17 @3 Kyoto JPN @4 2006-08-20 |
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<term>Magnetic semiconductors</term>
<term>Nuclear magnetic resonance</term>
<term>Ordering</term>
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<term>Spin fluctuations</term>
<term>Spin-lattice relaxation</term>
<term>Thulium tellurides</term>
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<term>Relaxation spin réseau</term>
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<term>Thulium tellurure</term>
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<front><div type="abstract" xml:lang="en">To elucidate from a microscopic point of view the initial evolution of spin fluctuations in TmTe from the semiconducting state at ambient pressure with an antiferroquadrupole ordering (T<sub>Q</sub>
= 1.8K) to the intermediate-valence metallic state at high pressures P≥2 GPa with a ferromagnetic (FM) ordering (T<sub>c</sub>
≃ 14 K), we have carried out <sup>125</sup>
Te-NMR study at pressures P = 0 and 0.9 GPa. The spin-lattice relaxation rate measurements revealed a pronounced increase of the staggered susceptibility below T≃ 14 K, in addition to the Curie-Weiss-type increase of the uniform susceptibility. Below ∼T<sup>*</sup>
, a wipe-out decrease of the NMR intensity and the finding of an unconventional NMR signal around ∼ 10 MHz that is insensitive to applied field lead to the conclusion that a field-induced short-range FM ordering caused by the competition of FM and antiferromagnetic fluctuations takes place. Pressure of 0.9 GPa hardly affects the anomalous NMR behaviors below <sup>∼</sup>
T<sup>*</sup>
, leading to speculate that the short-range FM ordering in the semiconducting state shares the origin with the long-range FM ordering at≃ 14K in the high-pressure metallic state.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Pressure effect on the competition between ferromagnetic and antiferromagnetic spin fluctuations in TmTe investigated by <sup>125</sup>
Te-NMR</s1>
</fA08>
<fA09 i1="01" i2="1" l="ENG"><s1>Proceedings of the 17th International Conference on Magnetism (ICM 2006), Kyoto, 20-25 August 2006. Part I (Chapters 1-2)</s1>
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<fA11 i1="01" i2="1"><s1>YAMAMOTO (A.)</s1>
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<fA11 i1="03" i2="1"><s1>MATSUMURA (T.)</s1>
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<fA12 i1="08" i2="1"><s1>ZHENG (G.-q.)</s1>
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<fA14 i1="01"><s1>Department of Material Science, Graduate School of Science and Technology, Kobe University</s1>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<fA14 i1="02"><s1>Department of Physics, Graduate School of Science, Tohoku University</s1>
<s2>Sendai 980-8578</s2>
<s3>JPN</s3>
<sZ>3 aut.</sZ>
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<sZ>5 aut.</sZ>
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</fA66>
<fC01 i1="01" l="ENG"><s0>To elucidate from a microscopic point of view the initial evolution of spin fluctuations in TmTe from the semiconducting state at ambient pressure with an antiferroquadrupole ordering (T<sub>Q</sub>
= 1.8K) to the intermediate-valence metallic state at high pressures P≥2 GPa with a ferromagnetic (FM) ordering (T<sub>c</sub>
≃ 14 K), we have carried out <sup>125</sup>
Te-NMR study at pressures P = 0 and 0.9 GPa. The spin-lattice relaxation rate measurements revealed a pronounced increase of the staggered susceptibility below T≃ 14 K, in addition to the Curie-Weiss-type increase of the uniform susceptibility. Below ∼T<sup>*</sup>
, a wipe-out decrease of the NMR intensity and the finding of an unconventional NMR signal around ∼ 10 MHz that is insensitive to applied field lead to the conclusion that a field-induced short-range FM ordering caused by the competition of FM and antiferromagnetic fluctuations takes place. Pressure of 0.9 GPa hardly affects the anomalous NMR behaviors below <sup>∼</sup>
T<sup>*</sup>
, leading to speculate that the short-range FM ordering in the semiconducting state shares the origin with the long-range FM ordering at≃ 14K in the high-pressure metallic state.</s0>
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<fC02 i1="03" i2="3"><s0>001B70E30M</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Effet pression</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Pressure effects</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Fluctuation spin</s0>
<s5>03</s5>
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<s5>03</s5>
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<s5>04</s5>
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<s5>05</s5>
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<s5>05</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Relación orden</s0>
<s5>05</s5>
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<fC03 i1="05" i2="3" l="FRE"><s0>Valence intermédiaire</s0>
<s5>06</s5>
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<fC03 i1="05" i2="3" l="ENG"><s0>Intermediate valence</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Haute pression</s0>
<s5>07</s5>
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<fC03 i1="06" i2="3" l="ENG"><s0>High pressure</s0>
<s5>07</s5>
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<fC03 i1="07" i2="3" l="FRE"><s0>Ferromagnétisme</s0>
<s5>08</s5>
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<fC03 i1="07" i2="3" l="ENG"><s0>Ferromagnetism</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Relaxation spin réseau</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Spin-lattice relaxation</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Loi Curie Weiss</s0>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Curie-Weiss law</s0>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Matériau ferromagnétique</s0>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Ferromagnetic materials</s0>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Thulium tellurure</s0>
<s2>NK</s2>
<s5>16</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Thulium tellurides</s0>
<s2>NK</s2>
<s5>16</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Semiconducteur magnétique</s0>
<s5>18</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Magnetic semiconductors</s0>
<s5>18</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>TmTe</s0>
<s4>INC</s4>
<s5>53</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>7550P</s0>
<s4>INC</s4>
<s5>60</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>7660</s0>
<s4>INC</s4>
<s5>61</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>7530M</s0>
<s4>INC</s4>
<s5>62</s5>
</fC03>
<fN21><s1>128</s1>
</fN21>
</pA>
<pR><fA30 i1="01" i2="1" l="ENG"><s1>ICM 2006 : International Conference on Magnetism</s1>
<s2>17</s2>
<s3>Kyoto JPN</s3>
<s4>2006-08-20</s4>
</fA30>
</pR>
</standard>
</inist>
</record>
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