Quasielastic neutron scattering of hydrated BaZr_{0.90}A_{0.10}O_{2.95} (A = Y and Sc)
| dc.creator | Karlsson, M. | |
| dc.creator | Matic, A. | |
| dc.creator | Engberg, D. | |
| dc.creator | Björketun, M. E. | |
| dc.creator | Koza, M. M. | |
| dc.creator | Ahmed, I. | |
| dc.creator | Wahnström, G. | |
| dc.creator | Berastegui, P. | |
| dc.creator | Börjesson, L. | |
| dc.creator | Eriksson, S. | |
| dc.date | 2008-02-07 | |
| dc.date.accessioned | 2026-07-07T09:19:14Z | |
| dc.date.available | 2026-07-07T09:19:14Z | |
| dc.description | Proton motions in hydrated proton conducting perovskites BaZr_{0.90}A_{0.10}O_{2.95} (A = Y and Sc) have been investigated using quasielastic neutron scattering. The results reveal a localized motion on the ps time scale and with an activation energy of ~10-30 meV, in both materials. The temperature dependence of the total mean square displacement of the protons suggests an onset of this motion at a temperature of about 300 K. Comparison of the QENS results to density functional theory calculations suggests that for both materials this motion can be ascribed to intra-octahedral proton transfers occurring close to a dopant atom. The low activation energy, more than ten times lower than the activation energy for the macroscopic proton conductivity, suggests that this motion is not the rate-limiting process for the long-range proton diffusion, i.e. it is not linked to the two materials significantly different proton conductivities. | |
| dc.description | 8 pages, 7 figures, 2 tables | |
| dc.identifier | https://arxiv.org/abs/0802.0924 | |
| dc.identifier | http://arxiv.org/abs/0802.0924 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/154316 | |
| dc.subject | Materials Science | |
| dc.title | Quasielastic neutron scattering of hydrated BaZr_{0.90}A_{0.10}O_{2.95} (A = Y and Sc) | |
| dc.type | text |