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<dc:title xml:lang="en">Temperature dependent spin wave study of magnetic properties and spin-polarized electron transport in Fe1-xVx and Co2MnSi epitaxial films</dc:title>
<dcterms:alternative xml:lang="fr">Étude par ondes de spin des propriétés magnétiques et électriques des alliages Fe1-xVx et Co2MnSi à température variable</dcterms:alternative>
<dc:subject xml:lang="fr">Transport électronique</dc:subject>
<dc:subject xml:lang="fr">Polarisation en spin</dc:subject>
<dc:subject xml:lang="fr">Fer</dc:subject>
<dc:subject xml:lang="fr">Alliage de Heusler</dc:subject>
<dc:subject xml:lang="fr">Onde de spin</dc:subject>
<dc:subject xml:lang="fr">Couche mince epitaxial</dc:subject>
<dc:subject xml:lang="en">Electron transport</dc:subject>
<dc:subject xml:lang="en">Spin-polarization</dc:subject>
<dc:subject xml:lang="en">Iron</dc:subject>
<dc:subject xml:lang="en">Heusler compound</dc:subject>
<dc:subject xml:lang="en">Spin wave</dc:subject>
<dc:subject xml:lang="en">Epitaxial thin films</dc:subject>
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<dcterms:abstract xml:lang="fr">Dans ce travail, nous étudions expérimentalement le transport électronique polarisé en spin dans des dispositifs nano-fabriqués à partir de films minces épitaxiaux de C"o" _2MnSi et de F"e" _(1-x) "V" _x. Le premier matériau est un alliage de Heusler n’ayant qu’une bande majoritaire de spin au niveau de Fermi, tandis que le second est un ferromagnétique faible ayant deux bandes de spin au niveau de Fermi. Notre principal outil expérimental est la technique du décalage Doppler des ondes de spin qui nous permet d'estimer le degré de polarisation en spin du courant P =(ρ↓-ρ↑)/(ρ↑+ρ↓) et de séparer les deux canaux de conduction. Pour C"o" _2MnSi, nous avons déterminé un transport électronique polarisé à 100% en spin en accord avec les estimations théoriques, ce qui nous donne un modèle de conduction relativement simple. Dans le cas du Fe, nous avons utilisé une variante dépendante de la température de notre technique expérimentale pour estimer une très haute polarisation en spin du courant (77-86%) dans la plage de température de 10 à 300 K. Cette observation contredit les considérations antérieures, qui, basées sur sa densité globale d'états, prédisent une faible polarisation en spin pour le fer. Enfin, nous avons utilisé nos mesures pour créer un modèle relativement simple afin de comprendre le rôle joué par les surfaces, les phonons ainsi que les magnons dans le transport électronique polarisé en spin dans le Fe.</dcterms:abstract>
<dcterms:abstract xml:lang="en">In this work we investigate experimentally the spin-polarized electron transport in nanofabricated devices from C"o" _2MnSi and F"e" _(1-x) "V" _x epitaxial thin films. The first material is a Heusler compound with only a majority spin band crossing the Fermi level, while the second is a weak-ferromagnet with two spin-bands at the Fermi level. Our main experimental tool is the spin wave Doppler shift technique which allows us to estimate the degree of spin-polarization of the current P =(ρ↓-ρ↑)/(ρ↑+ρ↓) and separate the two channels of conduction. For C"o" _2MnSi we determined a 100% spin-polarized electron transport in agreement with theoretical estimations that results in a relatively simple conduction model. In the case of Fe, we have used a temperature dependent variation of our experimental technique to estimate a very high spin-polarization of the current (77-86%) in the temperature range 10-300K. This observation contradicts early considerations, which, based on its global density of states, predicts a week spin polarization for iron. Finally, we used our measurements to create a relatively simple model to understand the role played by surfaces, phonons and magnons in the spin-polarized electron transport in Fe.</dcterms:abstract>
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