Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation

Effective control of magnetic anisotropy is important for developing spintronic devices. In this work, we performed a case study of stacking periods (N)-mediated reorientation of lateral magnetic anisotropy in ultrathin La0.67Ca0.33MnO3/SrRuO3 superlattices. As N increases from 1 to 15, the magnetic...

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Main Authors: Lili Qu, Da Lan, Kexuan Zhang, Enda Hua, Binghui Ge, Liqiang Xu, Feng Jin, Guanyin Gao, Lingfei Wang, Wenbin Wu
Format: Article
Language:English
Published: AIP Publishing LLC 2021-07-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0052109
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spelling doaj-93a43356b4dd40d6a93f635154c378632021-08-04T13:18:51ZengAIP Publishing LLCAIP Advances2158-32262021-07-01117075001075001-710.1063/5.0052109Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulationLili Qu0Da Lan1Kexuan Zhang2Enda Hua3Binghui Ge4Liqiang Xu5Feng Jin6Guanyin Gao7Lingfei Wang8Wenbin Wu9Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaInstitutes of Physical Science and Information Technology, Anhui University, Hefei 230601, ChinaInstitutes of Physical Science and Information Technology, Anhui University, Hefei 230601, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaHefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei 230026, ChinaEffective control of magnetic anisotropy is important for developing spintronic devices. In this work, we performed a case study of stacking periods (N)-mediated reorientation of lateral magnetic anisotropy in ultrathin La0.67Ca0.33MnO3/SrRuO3 superlattices. As N increases from 1 to 15, the magnetic easy-axis switches from the orthorhombic [010] to [100]-axis. The maximum anisotropy constant of the superlattice (SL) (N = 15) reaches −1.83 × 105 erg/cm3. X-ray absorption spectroscopy and x-ray linear dichroism further suggest that the observed changes in lateral magnetic anisotropy are driven by in-plane orbital polarization. For SLs with small N, anisotropic strain-induced orbital polarization along the b-axis can result in the [010]-oriented magnetic easy axis. For SLs with large N, the dimension crossover from 2-dimension to 3-dimension could enhance the hybridization of Ru t2g and Mn dx2−y2 orbitals, which can compete with the strain effect and switch the magnetic easy axis to [100]. Our results suggest a potential strategy for engineering magnetic anisotropy through the cooperation of strain engineering and interfacial orbital engineering.http://dx.doi.org/10.1063/5.0052109
collection DOAJ
language English
format Article
sources DOAJ
author Lili Qu
Da Lan
Kexuan Zhang
Enda Hua
Binghui Ge
Liqiang Xu
Feng Jin
Guanyin Gao
Lingfei Wang
Wenbin Wu
spellingShingle Lili Qu
Da Lan
Kexuan Zhang
Enda Hua
Binghui Ge
Liqiang Xu
Feng Jin
Guanyin Gao
Lingfei Wang
Wenbin Wu
Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
AIP Advances
author_facet Lili Qu
Da Lan
Kexuan Zhang
Enda Hua
Binghui Ge
Liqiang Xu
Feng Jin
Guanyin Gao
Lingfei Wang
Wenbin Wu
author_sort Lili Qu
title Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
title_short Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
title_full Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
title_fullStr Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
title_full_unstemmed Continuous tunable lateral magnetic anisotropy in La0.67Ca0.33MnO3/SrRuO3 superlattices by stacking period-modulation
title_sort continuous tunable lateral magnetic anisotropy in la0.67ca0.33mno3/srruo3 superlattices by stacking period-modulation
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2021-07-01
description Effective control of magnetic anisotropy is important for developing spintronic devices. In this work, we performed a case study of stacking periods (N)-mediated reorientation of lateral magnetic anisotropy in ultrathin La0.67Ca0.33MnO3/SrRuO3 superlattices. As N increases from 1 to 15, the magnetic easy-axis switches from the orthorhombic [010] to [100]-axis. The maximum anisotropy constant of the superlattice (SL) (N = 15) reaches −1.83 × 105 erg/cm3. X-ray absorption spectroscopy and x-ray linear dichroism further suggest that the observed changes in lateral magnetic anisotropy are driven by in-plane orbital polarization. For SLs with small N, anisotropic strain-induced orbital polarization along the b-axis can result in the [010]-oriented magnetic easy axis. For SLs with large N, the dimension crossover from 2-dimension to 3-dimension could enhance the hybridization of Ru t2g and Mn dx2−y2 orbitals, which can compete with the strain effect and switch the magnetic easy axis to [100]. Our results suggest a potential strategy for engineering magnetic anisotropy through the cooperation of strain engineering and interfacial orbital engineering.
url http://dx.doi.org/10.1063/5.0052109
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