Emergent half-metal with mixed structural order in (111)-oriented (LaMnO₃)₂ₙ|(SrMnO₃)ₙ superlattices
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<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:creator>Cossu, Fabrizio</dc:creator>
<dc:creator>Alves Do Nascimento, Jùlio</dc:creator>
<dc:creator>Cavill, Stuart A.</dc:creator>
<dc:creator>Di Marco, Igor</dc:creator>
<dc:creator>Lazarov, Vlado K.</dc:creator>
<dc:creator>Kim, Heung-Sik</dc:creator>
<dc:date>2024-05-23</dc:date>
<dc:description>Using first-principles techniques, we study the structural, magnetic, and electronic properties of (111)-oriented (LaMnO₃)₂ₙ|(SrMnO₃)ₙ superlattices of varying thickness (n=2,4,6). We find that the properties of the thinnest superlattice (n=2) are similar to the celebrated half-metallic ferromagnetic alloy La2/3Sr1/3MnO₃, with quenched Jahn-Teller distortions. At intermediate thickness (n=4), the a⁻a⁻a⁻ tilting pattern transitions to the a⁻a⁻c⁺ tilting pattern, driven by the lattice degrees of freedom in the LaMnO₃ region. The emergence of the Jahn-Teller modes and the spatial extent needed for their development play a key role in this structural transition. For the largest thickness considered (n=6), we unveil an emergent separation of Jahn-Teller and volume-breathing orders in the ground-state structure with the a⁻a⁻c⁺ tilting pattern, whereas it vanishes in the antiferromagnetic configurations. The ground state of all superlattices is half-metallic ferromagnetic, not affected by the underlying series of structural transitions. Overall, these results outline a thickness-induced crossover between the physical properties of bulk La2/3Sr1/3MnO₃ and bulk LaMnO₃. The dataset includes the fully relaxed atomic positions of the most favorable tilting patterns, as well as the main output files of the electronic structure calculations. Selected files for the density of states are also included.</dc:description>
<dc:identifier>https://archive.materialscloud.org/record/2024.78</dc:identifier>
<dc:identifier>doi:10.24435/materialscloud:4f-j1</dc:identifier>
<dc:identifier>mcid:2024.78</dc:identifier>
<dc:identifier>oai:materialscloud.org:2195</dc:identifier>
<dc:language>en</dc:language>
<dc:publisher>Materials Cloud</dc:publisher>
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:rights>Creative Commons Attribution 4.0 International https://creativecommons.org/licenses/by/4.0/legalcode</dc:rights>
<dc:subject>H2020</dc:subject>
<dc:subject>DFT</dc:subject>
<dc:subject>DFT+U</dc:subject>
<dc:subject>Oxide heterostructures</dc:subject>
<dc:subject>Electronic properties</dc:subject>
<dc:subject>Magnetic properties</dc:subject>
<dc:title>Emergent half-metal with mixed structural order in (111)-oriented (LaMnO₃)₂ₙ|(SrMnO₃)ₙ superlattices</dc:title>
<dc:type>Dataset</dc:type>
</oai_dc:dc>