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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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Rosendal, Victor
Technical University of Denmark
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Topics
Publications (4/4 displayed)
- 2024Electron-vacancy scattering in SrNbO3 and SrTiO3
- 2024Electron-vacancy scattering in SrNbO 3 and SrTiO 3 :A density functional theory study with nonequilibrium Green's functions
- 2024Deconvolution of heat sources for application in thermoelectric micro four-point probe measurementscitations
- 2023Octahedral distortions in SrNbO3citations
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article
Octahedral distortions in SrNbO3
Abstract
Strontium niobate has triggered a lot of interest as a transparent conductor and as a possible realization of a correlated Dirac semimetal. Using the lattice parameters as a tunable knob, the energy landscape of octahedral tilting was mapped using density functional theory calculations. We find that biaxial compressive strain induces tilting around the out-of-plane axis, while tensile strain induces tilting around the two in-plane axes. The two competing distorted structures for compressive strain show semi-Dirac dispersions above the Fermi level in their electronic structure. Our density functional theory calculations combined with dynamical mean field theory reveal that dynamical correlations downshift these semi-Dirac-like cones towards the Fermi energy. More generally, our study reveals that the competition between the <i>in-phase</i> and <i>out-of-phase</i> tilting in SrNbO<sub>3</sub> provides a new degree of freedom that allows for tuning the thermoelectric and optical properties. We show how the tilt angle and mode are reflected in the behavior of the Seebeck coefficient and the plasma frequency due to changes in the band structure.