Half-Metallic Ferromagnetism in the Heusler Compound Co\(_2\)FeSi revealed by Resistivity, Magnetoresistance, and Anomalous Hall Effect measurements
We present electrical transport data for single-crystalline Co\(_2\)FeSi which provide clear-cut evidence that this Heusler compound is truly a half-metallic ferromagnet, i.e. it possesses perfect spin-polarization. More specifically, the temperature dependence of \(\rho\) is governed by electron sc...
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creator | Bombor, Dirk Blum, Christian G F Volkonskiy, Oleg Rodan, Steven Wurmehl, Sabine Hess, Christian Büchner, Bernd |
description | We present electrical transport data for single-crystalline Co\(_2\)FeSi which provide clear-cut evidence that this Heusler compound is truly a half-metallic ferromagnet, i.e. it possesses perfect spin-polarization. More specifically, the temperature dependence of \(\rho\) is governed by electron scattering off magnons which are thermally excited over a sizeable gap \(\Delta\approx 100 K\) (\(\sim 9 meV\)) separating the electronic majority states at the Fermi level from the unoccupied minority states. As a consequence, electron-magnon scattering is only relevant at \(T\gtrsim\Delta\) but freezes out at lower temperatures, i.e., the spin-polarization of the electrons at the Fermi level remains practically perfect for \(T\lesssim\Delta\). The gapped magnon population has a decisive influence on the magnetoresistance and the anomalous Hall effect (AHE): i) The magnetoresistance changes its sign at \(T\sim 100 K\), ii) the anomalous Hall coefficient is strongly temperature dependent at \(T\gtrsim 100 K\) and compatible with Berry phase related and/or side-jump electronic deflection, whereas it is practically temperature-independent at lower temperatures. |
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More specifically, the temperature dependence of \(\rho\) is governed by electron scattering off magnons which are thermally excited over a sizeable gap \(\Delta\approx 100 K\) (\(\sim 9 meV\)) separating the electronic majority states at the Fermi level from the unoccupied minority states. As a consequence, electron-magnon scattering is only relevant at \(T\gtrsim\Delta\) but freezes out at lower temperatures, i.e., the spin-polarization of the electrons at the Fermi level remains practically perfect for \(T\lesssim\Delta\). The gapped magnon population has a decisive influence on the magnetoresistance and the anomalous Hall effect (AHE): i) The magnetoresistance changes its sign at \(T\sim 100 K\), ii) the anomalous Hall coefficient is strongly temperature dependent at \(T\gtrsim 100 K\) and compatible with Berry phase related and/or side-jump electronic deflection, whereas it is practically temperature-independent at lower temperatures.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1207.6611</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Electromagnetism ; Electron spin ; Fermi level ; Ferromagnetism ; Hall effect ; Iron silicide ; Magnetoresistance ; Magnetoresistivity ; Magnons ; Polarization (spin alignment) ; Scattering ; Single crystals ; Temperature ; Temperature dependence</subject><ispartof>arXiv.org, 2012-07</ispartof><rights>2012. 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The gapped magnon population has a decisive influence on the magnetoresistance and the anomalous Hall effect (AHE): i) The magnetoresistance changes its sign at \(T\sim 100 K\), ii) the anomalous Hall coefficient is strongly temperature dependent at \(T\gtrsim 100 K\) and compatible with Berry phase related and/or side-jump electronic deflection, whereas it is practically temperature-independent at lower temperatures.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1207.6611</doi><oa>free_for_read</oa></addata></record> |
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subjects | Electromagnetism Electron spin Fermi level Ferromagnetism Hall effect Iron silicide Magnetoresistance Magnetoresistivity Magnons Polarization (spin alignment) Scattering Single crystals Temperature Temperature dependence |
title | Half-Metallic Ferromagnetism in the Heusler Compound Co\(_2\)FeSi revealed by Resistivity, Magnetoresistance, and Anomalous Hall Effect measurements |
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