TY - JOUR
T1 - Re-induced raman active modes in HgBa2Can-1CunO2n+2+δ compounds
AU - Poulakis, N.
AU - Lampakis, D.
AU - Liarokapis, E.
AU - Yoshikawa, Akira
AU - Shimoyama, Jun Ich
AU - Kishio, Kohji
AU - Peacock, G. B.
AU - Hodges, J. P.
AU - Gameson, I.
AU - Edwards, P. P.
AU - Panagopoulos, C.
PY - 1999
Y1 - 1999
N2 - 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.
AB - 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.
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U2 - 10.1103/PhysRevB.60.3244
DO - 10.1103/PhysRevB.60.3244
M3 - Article
AN - SCOPUS:0343973192
SN - 1098-0121
VL - 60
SP - 3244
EP - 3251
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
ER -