| People | Locations | Statistics |
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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Mertig, Ingrid
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (27/27 displayed)
- 2023Controlled electronic and magnetic landscape in self-assembled complex oxide heterostructures
- 2023Spin-polarized two-dimensional electron/hole gas at the interface of non-magnetic semiconducting half-Heusler compounds: Modified Slater-Pauling rule for half-metallicity at the interface
- 2023Atomic Scale Control of Spin Current Transmission at Interfaces
- 2023Controlled electronic and magnetic landscape in self‐assembled complex oxide heterostructurescitations
- 2023Controlled Electronic and Magnetic Landscape in Self‐Assembled Complex Oxide Heterostructurescitations
- 2023Atomic displacements enabling the observation of the anomalous Hall effect in a non-collinear antiferromagnet
- 2023Atomic Displacements Enabling the Observation of the Anomalous Hall Effect in a Non‐Collinear Antiferromagnetcitations
- 2023Generation of out-of-plane polarized spin current by spin swappingcitations
- 2023Generation of out-of-plane polarized spin current by spin swapping
- 2022Atomic scale control of spin current transmission at interfaces
- 2022Defect-induced magnetism in homoepitaxial SrTiO3
- 2022Defect-induced magnetism in homoepitaxial SrTiO3citations
- 2022Setting of the magnetic structure of chiral kagome antiferromagnets by a seeded spin-orbit torquecitations
- 2022Setting of the magnetic structure of chiral kagome antiferromagnets by a seeded spin-orbit torque
- 2021Broadband Terahertz Probes of Anisotropic Magnetoresistance Disentangle Extrinsic and Intrinsic Contributions
- 2021Broadband terahertz probes of anisotropic magnetoresistance disentangle extrinsic and intrinsic contributionscitations
- 2021Broadband terahertz probes of anisotropic magnetoresistance disentangle extrinsic and intrinsic contributionscitations
- 2020Half-Metal–Spin-Gapless-Semiconductor Junctions as a Route to the Ideal Diodecitations
- 2020Impact of crystalline anisotropy on the extrinsic spin Hall effect in ultrathin films
- 2020Determining the Rashba parameter from the bilinear magnetoresistance response in a two-dimensional electron gascitations
- 2019Proposal for Reconfigurable Magnetic Tunnel Diode and Transistorcitations
- 2016The 2016 oxide electronic materials and oxide interfaces roadmap
- 2016Nanostructure, thermoelectric properties, and transport theory of V2VI3 and V2VI3/IV-VI based superlattices and nanomaterialscitations
- 2013Spin Hall and spin Nernst effect in dilute ternary alloyscitations
- 2011Extrinsic and Intrinsic Contributions to the Spin Hall Effect of Alloys
- 2011Extrinsic and Intrinsic Contributions to the Spin Hall Effect of Alloyscitations
- 2009Spin polarization on Fermi surfaces of metals by the KKR methodcitations
Places of action
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article
Controlled Electronic and Magnetic Landscape in Self‐Assembled Complex Oxide Heterostructures
Abstract
<jats:title>Abstract</jats:title><jats:p>Complex oxide heterointerfaces contain a rich playground of novel physical properties and functionalities, which give rise to emerging technologies. Among designing and controlling the functional properties of complex oxide film heterostructures, vertically aligned nanostructure (VAN) films using a self‐assembling bottom‐up deposition method presents great promise in terms of structural flexibility and property tunability. Here, the bottom‐up self‐assembly is extended to a new approach using a mixture containing a 2Dlayer‐by‐layer film growth, followed by a 3D VAN film growth. In this work, the two‐phase nanocomposite thin films are based on LaAlO<jats:sub>3</jats:sub>:LaBO<jats:sub>3</jats:sub>, grown on a lattice‐mismatched SrTiO<jats:sub>3001</jats:sub> (001) single crystal. The 2D‐to‐3D transient structural assembly is primarily controlled by the composition ratio, leading to the coexistence of multiple interfacial properties, 2D electron gas, and magnetic anisotropy. This approach provides multidimensional film heterostructures which enrich the emergent phenomena for multifunctional applications.</jats:p>