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Isothermal section at 800°C of the ternary system Tm-Fe-Si

Identifieur interne : 002D00 ( Main/Merge ); précédent : 002C99; suivant : 002D01

Isothermal section at 800°C of the ternary system Tm-Fe-Si

Auteurs : M. Muller [Allemagne] ; H. Schmidt [Allemagne] ; H. F. Braun [Allemagne]

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RBID : Pascal:97-0478580

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English descriptors

Abstract

Copyright (c) 1997 Elsevier Science S.A. All rights reserved. The isothermal section at 800°C of the Tm-Fe-Si ternary phase diagram was investigated using X-ray diffractometry, metallographic analysis and EDX-microanalysis. We found eleven binary and at least nine ternary phases. For two ternary phases reported as Tm2Fe4Si9 with Y2Fe4Si9-type structure [1] and Tm3Fe2Si7 with Ho3Co2Si7-type structure [1] the composition could not be confirmed, but was found as Tm9±1Fe26±1Si65±3 and Tm21±1Fe18.5±1Si60.5±1. New ternary phases were found at compositions Tm30±1Fe12.8±1Si57.2±1, which could be indexed orthorhombic, Tm30±2Fe5±1Si65±3, Tm37±1Fe25±1Si38±1 and Tm40±1Fe19±1Si41±1. Two binary and four ternary phases are in equilibrium with the re-entrant superconducting compound Tm2Fe3Si5, which are FeSi, TmSi, TmFe2Si2, Tm21±1Fe18.5±1Si60.5±1, Tm9±1Fe26±1Si65±1 and Tm30±1Fe12.8±1Si57.2±1. The width of the homogeneity range of the Tm2Fe3Si5 phase was determined to 1.6±0.4 at.% at constant Tm concentration and to 0.5±0.15 at.% at constant Fe/Si-ratio.

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Pascal:97-0478580

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<term>Isothermal section</term>
<term>Metallography</term>
<term>Phase diagrams</term>
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<term>Space groups</term>
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<term>XRD</term>
<term>Métallographie</term>
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<term>Composé intermétallique</term>
<term>Etude expérimentale</term>
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<div type="abstract" xml:lang="en">Copyright (c) 1997 Elsevier Science S.A. All rights reserved. The isothermal section at 800°C of the Tm-Fe-Si ternary phase diagram was investigated using X-ray diffractometry, metallographic analysis and EDX-microanalysis. We found eleven binary and at least nine ternary phases. For two ternary phases reported as Tm
<sub>2</sub>
Fe
<sub>4</sub>
Si
<sub>9</sub>
with Y
<sub>2</sub>
Fe
<sub>4</sub>
Si
<sub>9</sub>
-type structure [1] and Tm
<sub>3</sub>
Fe
<sub>2</sub>
Si
<sub>7</sub>
with Ho
<sub>3</sub>
Co
<sub>2</sub>
Si
<sub>7</sub>
-type structure [1] the composition could not be confirmed, but was found as Tm
<sub>9±1</sub>
Fe
<sub>26±1</sub>
Si
<sub>65±3</sub>
and Tm
<sub>21±1</sub>
Fe
<sub>18.5±1</sub>
Si
<sub>60.5±1</sub>
. New ternary phases were found at compositions Tm
<sub>30±1</sub>
Fe
<sub>12.8±1</sub>
Si
<sub>57.2±1</sub>
, which could be indexed orthorhombic, Tm
<sub>30±2</sub>
Fe
<sub>5±1</sub>
Si
<sub>65±3</sub>
, Tm
<sub>37±1</sub>
Fe
<sub>25±1</sub>
Si
<sub>38±1</sub>
and Tm
<sub>40±1</sub>
Fe
<sub>19±1</sub>
Si
<sub>41±1</sub>
. Two binary and four ternary phases are in equilibrium with the re-entrant superconducting compound Tm
<sub>2</sub>
Fe
<sub>3</sub>
Si
<sub>5</sub>
, which are FeSi, TmSi, TmFe
<sub>2</sub>
Si
<sub>2</sub>
, Tm
<sub>21±1</sub>
Fe
<sub>18.5±1</sub>
Si
<sub>60.5±1</sub>
, Tm
<sub>9±1</sub>
Fe
<sub>26±1</sub>
Si
<sub>65±1</sub>
and Tm
<sub>30±1</sub>
Fe
<sub>12.8±1</sub>
Si
<sub>57.2±1</sub>
. The width of the homogeneity range of the Tm
<sub>2</sub>
Fe
<sub>3</sub>
Si
<sub>5</sub>
phase was determined to 1.6±0.4 at.% at constant Tm concentration and to 0.5±0.15 at.% at constant Fe/Si-ratio.</div>
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