Phase Change Observed in Ultrathin Ba0.5Sr0.5TiO3 Films by in-situ Resonant Photoemission Spectroscopy
| dc.creator | Lin, Y. -H. | |
| dc.creator | Terai, K. | |
| dc.creator | Wadati, H. | |
| dc.creator | Kobayashi, M. | |
| dc.creator | Takizawa, M. | |
| dc.creator | Hwang, J. I. | |
| dc.creator | Fujimori, A. | |
| dc.creator | Nan, C. -W. | |
| dc.creator | Li, J. -F. | |
| dc.creator | Fujimori, S. -I. | |
| dc.creator | Okane, T. | |
| dc.creator | Saitoh, Y. | |
| dc.creator | Kobayashi, K. | |
| dc.date | 2007-05-24 | |
| dc.date.accessioned | 2026-07-07T08:09:23Z | |
| dc.date.available | 2026-07-07T08:09:23Z | |
| dc.description | Epitaxial Ba0.5Sr0.5TiO3 thin films were prepared on Nb-doped SrTiO3 (100)substrates by the pulsed laser deposition technique, and were studied by measuring the Ti 2p - 3d resonant photoemission spectra in the valence-band region as a function of film thickness, both at room temperature and low temperature. Our results demonstrated an abrupt variation in the spectral structures between 2.8 nm (~7 monolayers) and 2.0 nm (~5 monolayers) Ba0.5Sr0.5TiO3 films, suggesting that there exists a critical thickness for phase change in the range of 2.0 nm to 2.8 nm. This may be ascribed mainly to the intrinsic size effects. | |
| dc.description | 13 pages, 4 figures | |
| dc.identifier | https://arxiv.org/abs/0705.3675 | |
| dc.identifier | http://arxiv.org/abs/0705.3675 | |
| dc.identifier | Appl. Phys. Lett. 90, 222909 (2007) | |
| dc.identifier | doi:10.1063/1.2745249 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/131525 | |
| dc.subject | Materials Science | |
| dc.title | Phase Change Observed in Ultrathin Ba0.5Sr0.5TiO3 Films by in-situ Resonant Photoemission Spectroscopy | |
| dc.type | text |