Quantum paraelectric behavior of pyrochlore PMN
| dc.creator | Kamba, S. | |
| dc.creator | Nuzhnyy, D. | |
| dc.creator | Denisov, S. | |
| dc.creator | Veljko, S. | |
| dc.creator | Bovtun, V. | |
| dc.creator | Savinov, M. | |
| dc.creator | Petzelt, J. | |
| dc.creator | Kalnberga, M. | |
| dc.creator | Sternberg, A. | |
| dc.date | 2007-03-06 | |
| dc.date | 2007-07-12 | |
| dc.date.accessioned | 2026-07-07T08:31:54Z | |
| dc.date.available | 2026-07-07T08:31:54Z | |
| dc.description | Pb_1.83Mg_0.29Nb_1.71O_6.39 (PMN) crystallizing in a cubic pyrochlore structure exhibits, as the first dielectrics with pyrochlore structure, typical feature of quantum paraelectrics - its permittivity continuously increases on cooling and levels off below ~ 30K, without any signature of a structural phase transition. Broad-band dielectric spectra do not show any dielectric dispersion in the real part of permittivity up to 8.8 GHz. THz and infrared spectra reveal a soft polar optic mode which is responsible for the temperature dependence of the permittivity. The leveling-off of the permittivity at low temperatures obeys the Barrett formula and the fitted vibrational zero-point energy 1/(2*k_B*T_1) corresponds to the measured soft mode frequency. The number of observed infrared phonons exceeds that predicted from the factor-group analysis which indicates that the structure is at least locally non-cubic. | |
| dc.description | subm. to PRB, revised version according to referees' reports | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0703159 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0703159 | |
| dc.identifier | Phys. Rev. B 76, 054125 (2007) | |
| dc.identifier | doi:10.1103/PhysRevB.76.054125 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/138641 | |
| dc.subject | Materials Science | |
| dc.title | Quantum paraelectric behavior of pyrochlore PMN | |
| dc.type | text |