Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures
In this work we report on the generation and transport of pure spin currents in La2/3Sr1/3MnO3(LSMO)/NiO/Pt heterostructures. Pure spin currents, generated by means of spin pumping in the LSMO layer, are transmitted through the NiO layer and detected by measuring the transverse voltage signal genera...
| Autores: | , , , , , , , |
|---|---|
| Tipo de recurso: | artículo |
| Estado: | Versión aceptada para publicación |
| Fecha de publicación: | 2025 |
| País: | España |
| Institución: | Consejo Superior de Investigaciones Científicas (CSIC) |
| Repositorio: | DIGITAL.CSIC. Repositorio Institucional del CSIC |
| OAI Identifier: | oai:digital.csic.es:10261/382028 |
| Acceso en línea: | http://hdl.handle.net/10261/382028 https://api.elsevier.com/content/abstract/scopus_id/85208334804 |
| Access Level: | acceso abierto |
| Palabra clave: | Antiferromagnets Complex oxides heterostructures Inverse spin Hall effect Spin currents transmission Spin pumping |
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Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| title |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| spellingShingle |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures Chen, Shoulong Antiferromagnets Complex oxides heterostructures Inverse spin Hall effect Spin currents transmission Spin pumping |
| title_short |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| title_full |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| title_fullStr |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| title_full_unstemmed |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| title_sort |
Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructures |
| dc.creator.none.fl_str_mv |
Chen, Shoulong Pomar, Alberto Balcells, Lluis Konstantinovic, Zorica Frontera, Carlos Magén, César Mestres, Narcís Martínez Perea, Benjamín |
| author |
Chen, Shoulong |
| author_facet |
Chen, Shoulong Pomar, Alberto Balcells, Lluis Konstantinovic, Zorica Frontera, Carlos Magén, César Mestres, Narcís Martínez Perea, Benjamín |
| author_role |
author |
| author2 |
Pomar, Alberto Balcells, Lluis Konstantinovic, Zorica Frontera, Carlos Magén, César Mestres, Narcís Martínez Perea, Benjamín |
| author2_role |
author author author author author author author |
| dc.contributor.none.fl_str_mv |
Agencia Estatal de Investigación (España) Ministerio de Ciencia, Innovación y Universidades (España) China Scholarship Council European Commission #NODATA# #NODATA# #NODATA# #NODATA# #NODATA# #NODATA# #NODATA# #NODATA# Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72] |
| dc.subject.none.fl_str_mv |
Antiferromagnets Complex oxides heterostructures Inverse spin Hall effect Spin currents transmission Spin pumping |
| topic |
Antiferromagnets Complex oxides heterostructures Inverse spin Hall effect Spin currents transmission Spin pumping |
| description |
In this work we report on the generation and transport of pure spin currents in La2/3Sr1/3MnO3(LSMO)/NiO/Pt heterostructures. Pure spin currents, generated by means of spin pumping in the LSMO layer, are transmitted through the NiO layer and detected by measuring the transverse voltage signal generated by the inverse spin Hall effect (ISHE) in the Pt layer. The spin current transmission is studied as a function of the NiO thickness and temperature. NiO layers grown at room temperature are polycrystalline and their microstructural and magnetic features clearly depend on thickness. Scanning transmission electron microscopy techniques revealed that homogeneous conformal coating of the LSMO layer is only achieved for NiO layer thicknesses above about 2 nm. Below this critical thickness the NiO layer is discontinuous and its main role would be to disturb the LSMO/Pt interface causing it to behave as something similar to an insulating barrier. Magnetic measurements indicate that NiO layers are paramagnetic (PM) well below room temperature. In agreement with these observations, the amplitude of the ISHE voltage signal decreases monotonically on lowering temperature and makes evident that there are two spin conduction regimes as a function of the NiO layer thickness with different spin diffusion lengths. For thin discontinuous NiO layers a spin diffusion length of λSDL≈0.8 nm is found, which is slightly larger than typical values found for insulating barriers, but definitely smaller than λSDL≈3.8 nm found for NiO layer thickness above 2 nm. The latter being similar to λSDL previously reported for epitaxial NiO layers. Our findings indicate that inserting a PM NiO insulating layer of optimal thickness improves the spin transparency of the LSMO/Pt interface. Additionally, the results suggest that spin conduction through the NiO layer is likely driven by magnetic correlations and short-range thermal magnons. |
| publishDate |
2025 |
| dc.date.none.fl_str_mv |
2025 2025 2025 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article http://purl.org/coar/resource_type/c_6501 Postprint info:eu-repo/semantics/acceptedVersion |
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article |
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acceptedVersion |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10261/382028 https://api.elsevier.com/content/abstract/scopus_id/85208334804 |
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http://hdl.handle.net/10261/382028 https://api.elsevier.com/content/abstract/scopus_id/85208334804 |
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Inglés |
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Inglés |
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#PLACEHOLDER_PARENT_METADATA_VALUE# #PLACEHOLDER_PARENT_METADATA_VALUE# #PLACEHOLDER_PARENT_METADATA_VALUE# #PLACEHOLDER_PARENT_METADATA_VALUE# info:eu-repo/grantAgreement/AEI/Plan Estatal de investigación Científica y Técnica y de Innovación 2021-2023/CEX2023-001263-S info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2021-2023/PID2021-128410OB-I00 info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2021-2023/PID2021-124680OB-I00 info:eu-repo/grantAgreement/MICINN/Plan Estatal de investigación Científica y Técnica y de Innovación 2021-2023/PID2021–124680OB-I00 Journal of Alloys and Compounds The underlying dataset has been published as supplementary material of the article in the publisher platform at DOI 10.1016/j.jallcom.2024.177453 http://doi.org/10.1016/j.jallcom.2024.177453 Sí |
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info:eu-repo/semantics/openAccess |
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openAccess |
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application/pdf |
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Elsevier |
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Elsevier |
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reponame:DIGITAL.CSIC. Repositorio Institucional del CSIC instname:Consejo Superior de Investigaciones Científicas (CSIC) |
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Spin conduction and interfacial effects in La2/3Sr1/3MnO3/NiO/Pt heterostructuresChen, ShoulongPomar, AlbertoBalcells, LluisKonstantinovic, ZoricaFrontera, CarlosMagén, CésarMestres, NarcísMartínez Perea, BenjamínAntiferromagnetsComplex oxides heterostructuresInverse spin Hall effectSpin currents transmissionSpin pumpingIn this work we report on the generation and transport of pure spin currents in La2/3Sr1/3MnO3(LSMO)/NiO/Pt heterostructures. Pure spin currents, generated by means of spin pumping in the LSMO layer, are transmitted through the NiO layer and detected by measuring the transverse voltage signal generated by the inverse spin Hall effect (ISHE) in the Pt layer. The spin current transmission is studied as a function of the NiO thickness and temperature. NiO layers grown at room temperature are polycrystalline and their microstructural and magnetic features clearly depend on thickness. Scanning transmission electron microscopy techniques revealed that homogeneous conformal coating of the LSMO layer is only achieved for NiO layer thicknesses above about 2 nm. Below this critical thickness the NiO layer is discontinuous and its main role would be to disturb the LSMO/Pt interface causing it to behave as something similar to an insulating barrier. Magnetic measurements indicate that NiO layers are paramagnetic (PM) well below room temperature. In agreement with these observations, the amplitude of the ISHE voltage signal decreases monotonically on lowering temperature and makes evident that there are two spin conduction regimes as a function of the NiO layer thickness with different spin diffusion lengths. For thin discontinuous NiO layers a spin diffusion length of λSDL≈0.8 nm is found, which is slightly larger than typical values found for insulating barriers, but definitely smaller than λSDL≈3.8 nm found for NiO layer thickness above 2 nm. The latter being similar to λSDL previously reported for epitaxial NiO layers. Our findings indicate that inserting a PM NiO insulating layer of optimal thickness improves the spin transparency of the LSMO/Pt interface. Additionally, the results suggest that spin conduction through the NiO layer is likely driven by magnetic correlations and short-range thermal magnons.This work has received funding from the State Investigation Agency, through the Severo Ochoa Programme for Centres of Excellence in R&D (CEX2023–001263-S) and “OXISOT” (PID2021–128410OB-I00) and “AMONANO” (PID2020–112914RB-I00) and HTSUPERFUN (PID2021–124680OB-I00) funded by MCIN/AEI/ 10.13039/501100011033 and by “ERDF A way of making Europe”, by the “European Union”. Shoulong Chen acknowledges financial support from the China Scholarship Council (CSC). This work has been performed in the framework of the Ph.D. program in Materials Science of the Universitat Autònoma de Barcelona (UAB), through the CSC/UAB Joint Scholarship program.With funding from the Spanish government through the ‘Severo Ochoa Centre of Excellence’ accreditation (CEX2023-001263-S).Peer reviewedElsevierAgencia Estatal de Investigación (España)Ministerio de Ciencia, Innovación y Universidades (España)China Scholarship CouncilEuropean Commission#NODATA##NODATA##NODATA##NODATA##NODATA##NODATA##NODATA##NODATA#Consejo Superior de Investigaciones Científicas [https://ror.org/02gfc7t72]202520252025info:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_6501Postprintinfo:eu-repo/semantics/acceptedVersionapplication/pdfhttp://hdl.handle.net/10261/382028https://api.elsevier.com/content/abstract/scopus_id/85208334804reponame:DIGITAL.CSIC. Repositorio Institucional del CSICinstname:Consejo Superior de Investigaciones Científicas (CSIC)Inglés#PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE##PLACEHOLDER_PARENT_METADATA_VALUE#info:eu-repo/grantAgreement/AEI/Plan Estatal de investigación Científica y Técnica y de Innovación 2021-2023/CEX2023-001263-Sinfo:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2021-2023/PID2021-128410OB-I00info:eu-repo/grantAgreement/AEI/Plan Estatal de Investigación Científica y Técnica y de Innovación 2021-2023/PID2021-124680OB-I00info:eu-repo/grantAgreement/MICINN/Plan Estatal de investigación Científica y Técnica y de Innovación 2021-2023/PID2021–124680OB-I00Journal of Alloys and CompoundsThe underlying dataset has been published as supplementary material of the article in the publisher platform at DOI 10.1016/j.jallcom.2024.177453http://doi.org/10.1016/j.jallcom.2024.177453Síinfo:eu-repo/semantics/openAccessoai:digital.csic.es:10261/3820282026-05-22T06:33:51Z |
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15,81155 |