Spin Hall magnetoresistance and spin Seebeck effect in Pt |CoCr <sub>2</sub> O <sub>4</sub> heterostructures

This study delves into spin current-induced phenomena, such as spin-Hall magnetoresistance and the spin Seebeck effect within Pt films deposited on a noncollinear magnet, CoCr <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>2</mml:mn></mml:msub> </mml:math> O <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>4</mml:mn></mml:msub> </mml:math> (CCO), particularly at low temperatures. Detailed investigation of the angular dependencies of spin Hall magnetoresistance (SMR) and spin Seebeck effect (SSE) was carried out. The temperature-dependent behavior of both SMR and SSE signals exhibits a discernible variation correlated with different magnetic phases of CCO. To distinguish the contributions arising from magnetic proximity effects, we conducted X-ray magnetic dichroism (XMCD) at the Pt-M <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>3</mml:mn></mml:msub> </mml:math> edge. XMCD data from Pt/CCO heterostructures suggest that any magnetic moment associated with Pt, if present, is below the detection limit. This supports the notion that the observed signals primarily stem from SMR and SSE. This study offers insights into spin-current-driven phenomena, paving the way for potential spintronic applications.

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Publication Details

Journal
Science and Technology of Advanced Materials
Published
2025-02-03
DOI
https://doi.org/10.1080/14686996.2025.2457320
Citations
1
Primary Topic
Multiferroics and related materials
Type
article
Field-Weighted Citation Impact
0.43

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article

Spin Hall magnetoresistance and spin Seebeck effect in Pt |CoCr 2 O 4 heterostructures

E. Pellegrin, Beatriz Noheda, Hans Huebl, Nynke Vlietstra et al.
1 citations
Science and Technology of Advanced Materials
Multiferroics and related materials
0.43
article

Spin Hall magnetoresistance and spin Seebeck effect in Pt |CoCr 2 O 4 heterostructures

E. Pellegrin, Beatriz Noheda, Hans Huebl, Nynke Vlietstra, Maxim Mostovoy, M. Kronseder, Aisha Aqeel, Javier Herrero‐Martín, V. Hari Babu, J. A. Heuver, C. H. Back
article en
1 citations

Abstract

This study delves into spin current-induced phenomena, such as spin-Hall magnetoresistance and the spin Seebeck effect within Pt films deposited on a noncollinear magnet, CoCr <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>2</mml:mn></mml:msub> </mml:math> O <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>4</mml:mn></mml:msub> </mml:math> (CCO), particularly at low temperatures. Detailed investigation of the angular dependencies of spin Hall magnetoresistance (SMR) and spin Seebeck effect (SSE) was carried out. The temperature-dependent behavior of both SMR and SSE signals exhibits a discernible variation correlated with different magnetic phases of CCO. To distinguish the contributions arising from magnetic proximity effects, we conducted X-ray magnetic dichroism (XMCD) at the Pt-M <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi> </mml:mi> <mml:mn>3</mml:mn></mml:msub> </mml:math> edge. XMCD data from Pt/CCO heterostructures suggest that any magnetic moment associated with Pt, if present, is below the detection limit. This supports the notion that the observed signals primarily stem from SMR and SSE. This study offers insights into spin-current-driven phenomena, paving the way for potential spintronic applications.

Science and Technology of Advanced MaterialsVol. 26(1)
Bavarian Academy of Sciences and Humanities (DE), University of Groningen (NL), University of Augsburg (DE), ALBA Synchrotron (Spain) (ES), Munich Center for Quantum Science and Technology (DE), University of Regensburg (DE), Technical University of Munich (DE)
Deutsche Forschungsgemeinschaft, Munich Center for Quantum Science and Technology
Openalex Percentile: Top 46%
Multiferroics and related materials
0.43
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