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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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Suzuki, Keigo
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Topics
Publications (7/7 displayed)
- 2013Effects of Sn2+ Ion Size on Sn Doped SrTiO3citations
- 2009Fabrication of well-dispersed barium titanate nanoparticles by the electrospray of a colloidal solutioncitations
- 2008Ferroelectric 90° domain structure in a thin film of BaTiO3 fine ceramics observed by 300kV electron holographycitations
- 2008Fabrication of Monodispersed Barium Titanate Nanoparticles with Narrow Size Distributioncitations
- 2006Dielectric Properties of BaTiO<sub>3</sub> Thin Films Prepared by Laser Ablationcitations
- 2005Optical Band Gap of Barium Titanate Nanoparticles Prepared by RF-plasma Chemical Vapor Depositioncitations
- 2005High Energy-Resolution Electron Energy-Loss Spectroscopy Study of Electronic Structures of Barium Titanate Nanocrystalscitations
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article
High Energy-Resolution Electron Energy-Loss Spectroscopy Study of Electronic Structures of Barium Titanate Nanocrystals
Abstract
<jats:p>High energy-resolution electron energy-loss spectra were obtained from barium titanate (BaTiO<jats:sub>3</jats:sub>) nanocrystals (BTNCs), which were synthesized by chemical vapor deposition using inductively coupled plasma. Onset energies of spectral intensities were 3.2 eV for 34 nm BTNCs and 3.5 eV for 6 nm BTNCs. This indicates an increase in the bandgap energy of BaTiO<jats:sub>3</jats:sub> with a decrease in crystal sizes. Those onset energies obtained from 90 nm specimen areas showed an excellent agreement with those estimated by previously reported optical measurements. Volume plasmon peaks were observed at 26.5 eV for 34 nm BTNCs and 25 eV for 6 nm BTNCs. Dielectric functions of the BTNCs were derived from loss-functions by Kramers–Kronig analysis using the refractivity of bulk BaTiO<jats:sub>3</jats:sub> (=2.4). The peaks of O 2p→Ti 3d (t<jats:sub>2g</jats:sub>) transitions in the imaginary part of dielectric function (<jats:italic>ε</jats:italic><jats:sub>2</jats:sub>) were observed at 3.3 eV for 34 nm BTNCs and 3.8 eV for 6 nm BTNCs. Those of O 2p→Ti 3d (e<jats:sub>g</jats:sub>) transitions were at 7.8 eV for 34 nm BTNCs and 6.6 eV for 6 nm BTNCs.</jats:p>