Emergent half-metal with mixed structural order in (111)-oriented (LaMnO$_3$)$_{2n}$|(SrMnO$_3$)$_n$ superlattices
Phys. Rev. B 109, 045435 (2024) Using first-principles techniques, we study the structural, magnetic and electronic properties of (111)-oriented (LaMnO$_3$)$_{2n}$$\vert$(SrMnO$_3$)$_{n}$ superlattices of varying thickness ($n=2,4,6$). We find that the properties of the thinnest superlattice ($n=2$)...
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Zusammenfassung: | Phys. Rev. B 109, 045435 (2024) Using first-principles techniques, we study the structural, magnetic and
electronic properties of (111)-oriented
(LaMnO$_3$)$_{2n}$$\vert$(SrMnO$_3$)$_{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
La$_{2/3}$Sr$_{1/3}$MnO$_3$, 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 LaMnO$_3$ 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
La$_{2/3}$Sr$_{1/3}$MnO$_3$ and bulk LaMnO$_3$. |
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DOI: | 10.48550/arxiv.2311.01081 |