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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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Petersen, Dirch Hjorth
Technical University of Denmark
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (33/33 displayed)
- 2024Electron-vacancy scattering in SrNbO3 and SrTiO3
- 2024Deconvolution of heat sources for application in thermoelectric micro four-point probe measurementscitations
- 2023Octahedral distortions in SrNbO3citations
- 2022Review of Micro- and Nanoprobe Metrology for Direct Electrical Measurements on Product Waferscitations
- 2022Determination of thermoelectric properties from micro four-point probe measurementscitations
- 2021Effective electrical resistivity in a square array of oriented square inclusionscitations
- 2019Exploring conductivity in ex-situ doped Si thin films as thickness approaches 5 nmcitations
- 2019Exploring conductivity in ex-situ doped Si thin films as thickness approaches 5 nmcitations
- 2017High temperature SU-8 pyrolysis for fabrication of carbon electrodescitations
- 2016Defect evolution and dopant activation in laser annealed Si and Gecitations
- 2016Defect evolution and dopant activation in laser annealed Si and Gecitations
- 2016Atomic Layer Deposition of Ruthenium with TiN Interface for Sub-10 nm Advanced Interconnects beyond Coppercitations
- 2016Atomic Layer Deposition of Ruthenium with TiN Interface for Sub-10 nm Advanced Interconnects beyond Coppercitations
- 2016Pyrolytic carbon microelectrodes for impedance based cell sensingcitations
- 2015Terahertz wafer-scale mobility mapping of graphene on insulating substrates without a gatecitations
- 2014Electrical characterization of sputtered ZnO:Al films with microprobe technique
- 2014Optimized Laser Thermal Annealing on Germanium for High Dopant Activation and Low Leakage Currentcitations
- 2014Optimized Laser Thermal Annealing on Germanium for High Dopant Activation and Low Leakage Currentcitations
- 2014Laser thermal annealing of Ge, optimized for highly activated dopants and diode ION/IOFF ratios
- 2012In-situ Ga doping of fully strained Ge1-xSnx heteroepitaxial layers grown on Ge(001) substratescitations
- 2012Activation and thermal stability of ultra-shallow B+-implants in Ge
- 2012Activation and thermal stability of ultra-shallow B + -implants in Gecitations
- 2012Effect of B + Flux on the electrical activation of ultra-shallow B + implants in Ge
- 2012Effect of B+ Flux on the electrical activation of ultra-shallow B+ implants in Ge
- 2011Ultra Shallow Arsenic Junctions in Germanium Formed by Millisecond Laser Annealingcitations
- 2011Ultra Shallow Arsenic Junctions in Germanium Formed by Millisecond Laser Annealingcitations
- 2010Customizable in situ TEM devices fabricated in freestanding membranes by focused ion beam millingcitations
- 2010Customizable in situ TEM devices fabricated in freestanding membranes by focused ion beam millingcitations
- 2010Study of submelt laser induced junction nonuniformities using Therma-Probecitations
- 2008Impact of multiple sub-melt laser scans on the activation and diffusion of shallow Boron junctionscitations
- 2008Comparative study of size dependent four-point probe sheet resistance measurement on laser annealed ultra-shallow junctionscitations
- 2008Epitaxial Integration of Nanowires in Microsystems by Local Micrometer Scale Vapor Phase Epitaxycitations
- 2002Simulated SAM A-scans on multilayer MEMS components
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article
Electron-vacancy scattering in SrNbO3 and SrTiO3
Abstract
Oxygen vacancies are often attributed to changes in the electronic transport for perovskite oxide materials (ABO<sub>3</sub>). Here, we use density functional theory coupled with nonequilibrium Green's functions to systematically investigate the influence of O vacancies and also <i>A</i>- and <i>B</i>-site vacancies, on the electronic transport as characterized by a scattering cross section. We consider SrNbO<sub>3</sub> and <i>n</i>-type SrTiO<sub>3</sub> and contrast results for bulk and thin film (slab) geometries. By varying the electron doping in SrTiO<sub>3</sub> we get insight into how the electron-vacancy scattering varies for different experimental conditions. We observe a significant increase in the scattering cross section (in units of square-lattice parameter <i>a</i><sup>2</sup>) from ≈0.5-2.5<i>a</i><sup>2</sup> per vacancy in SrNbO<sub>3</sub> and heavily doped SrTiO<sub>3</sub> to more than 9<i>a</i><sup>2</sup> in SrTiO<sub>3</sub> with 0.02 free carriers per unit cell. Furthermore, the scattering strength of O vacancies is enhanced in TiO<sub>2</sub> terminated surfaces by a factor of more than 6 in lowly doped SrTiO<sub>3</sub> compared to other locations in slabs and bulk systems. Interestingly, we also find that Sr vacancies go from being negligible scattering centers in SrNbO<sub>3</sub> and heavily doped SrTiO<sub>3</sub>, to having a large scattering cross section in weakly doped SrTiO<sub>3</sub>. We therefore conclude that the electron-vacancy scattering in these systems is sensitive to the combination of electron concentration and vacancy location.