dc.contributor.author |
Poulakis, N |
en |
dc.contributor.author |
Lampakis, D |
en |
dc.contributor.author |
Liarokapis, E |
en |
dc.contributor.author |
Yoshikawa, A |
en |
dc.contributor.author |
Shimoyama, J-I |
en |
dc.contributor.author |
Kishio, K |
en |
dc.contributor.author |
Peacock, GB |
en |
dc.contributor.author |
Hodges, JP |
en |
dc.contributor.author |
Gameson, I |
en |
dc.contributor.author |
Edwards, PP |
en |
dc.contributor.author |
Panagopoulos, C |
en |
dc.date.accessioned |
2014-03-01T01:15:07Z |
|
dc.date.available |
2014-03-01T01:15:07Z |
|
dc.date.issued |
1999 |
en |
dc.identifier.issn |
0163-1829 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/13353 |
|
dc.subject.classification |
Physics, Condensed Matter |
en |
dc.subject.other |
MERCURY-BASED SUPERCONDUCTOR |
en |
dc.subject.other |
NEUTRON POWDER DIFFRACTION |
en |
dc.subject.other |
HG-BASED SUPERCONDUCTORS |
en |
dc.subject.other |
T-C |
en |
dc.subject.other |
CRYSTAL-STRUCTURE |
en |
dc.subject.other |
THERMAL-STABILITY |
en |
dc.subject.other |
HGBA2CUO4+DELTA |
en |
dc.subject.other |
HGBA2CA2CU3O8+DELTA |
en |
dc.subject.other |
SPECTRA |
en |
dc.subject.other |
OXYGEN |
en |
dc.title |
Re-induced Raman active modes in HgBa2Can-1CunO2n+2+δ compounds |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1103/PhysRevB.60.3244 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1103/PhysRevB.60.3244 |
en |
heal.language |
English |
en |
heal.publicationDate |
1999 |
en |
heal.abstract |
A comparative Raman study of Re-free and Re-doped HgBa2Can-1CunO2n+2+δ with n=1,3,4,5 is presented in an attempt to further clarify the structural and phononic modifications brought about by Re substitution. A number of extra high-frequency phonon peaks show up in the spectra of the Re-doped samples and are attributed to the oxygen modes of a strongly bound, almost decoupled ReO6 octahedron. As regards the apex oxygen in the Hg site, a clear transfer of spectral weight from the 590 to the 570 cm-1 apex phonon band is observed upon Re substitution. Such a change may well be accounted for assuming increased excess oxygen content for the Re-doped samples. Another interesting result is the enhancement upon Re doping of a narrow peak probably attributed to c-axis vibrations of Ba whose frequency shows a distinctive change with the number n of the CuO2 layers, providing an easy way to identify the various phases in a sample. ©1999 The American Physical Society. |
en |
heal.publisher |
AMERICAN PHYSICAL SOC |
en |
heal.journalName |
Physical Review B - Condensed Matter and Materials Physics |
en |
dc.identifier.doi |
10.1103/PhysRevB.60.3244 |
en |
dc.identifier.isi |
ISI:000081986300055 |
en |
dc.identifier.volume |
60 |
en |
dc.identifier.issue |
5 |
en |
dc.identifier.spage |
3244 |
en |
dc.identifier.epage |
3251 |
en |