TY - JOUR
T1 - Change in phonon Raman spectra of Bi2Sr2Ca1 - xYxCu2O8 + d induced by hole filling and implications for phonon assignments
AU - Osada, M.
AU - Kakihana, M.
AU - Käll, M.
AU - Börjesson, L.
AU - Yashima, M.
AU - Yoshimura, M.
PY - 1996/10/1
Y1 - 1996/10/1
N2 - The phonon Raman spectra of Bi2Sr2Ca1 - xYxCu2O8 + d (x = 0-1) have been investigated in a number of well-defined single crystal and polycrystalline samples. From the polarization and Y doping dependence, and from a comparison with previous reports on Bi-based cuprates, we identify the (6A1g + 1B1g) symmetry modes that are Raman allowed within the ideal body-centered tetragonal unit-cell. The vibrational modes that involve atoms in the CuO5 pyramid exhibit drastic changes with increasing Y doping: the bridging-oxygen phonon softens strongly, whereas the CuO2-plane phonons both harden and increase in intensity with increasing Y content. Although the intensity increases can be attributed to the reduced metallic screening in the hole-depleted Y doped samples, the phonon frequency variations are mainly due to the structural changes induced by the decrease in the average Ca/Y ion radius.
AB - The phonon Raman spectra of Bi2Sr2Ca1 - xYxCu2O8 + d (x = 0-1) have been investigated in a number of well-defined single crystal and polycrystalline samples. From the polarization and Y doping dependence, and from a comparison with previous reports on Bi-based cuprates, we identify the (6A1g + 1B1g) symmetry modes that are Raman allowed within the ideal body-centered tetragonal unit-cell. The vibrational modes that involve atoms in the CuO5 pyramid exhibit drastic changes with increasing Y doping: the bridging-oxygen phonon softens strongly, whereas the CuO2-plane phonons both harden and increase in intensity with increasing Y content. Although the intensity increases can be attributed to the reduced metallic screening in the hole-depleted Y doped samples, the phonon frequency variations are mainly due to the structural changes induced by the decrease in the average Ca/Y ion radius.
KW - Hole-filling effect
KW - Low-temperature Raman measurement
KW - Phonon assignment
KW - Polarized Raman measurement
KW - Single crystal
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U2 - 10.1016/S0921-5107(96)01634-0
DO - 10.1016/S0921-5107(96)01634-0
M3 - Article
AN - SCOPUS:0030260362
VL - 41
SP - 107
EP - 110
JO - Materials Science and Engineering B: Solid-State Materials for Advanced Technology
JF - Materials Science and Engineering B: Solid-State Materials for Advanced Technology
SN - 0921-5107
IS - 1
ER -