TY - JOUR
T1 - Raman-active phonons in Bi2Sr2-xLaxCuO6+d
T2 - Phonon assignment and charge-redistribution effects
AU - Osada, Minoru
AU - Kakihana, Masato
AU - Käll, Mikael
AU - Börjesson, Lars
AU - Inoue, Atsuyoshi
AU - Yashima, Masatomo
PY - 1997/8/1
Y1 - 1997/8/1
N2 - Phonon Raman spectra of Bi2Sr2-xLaxCuO6+d single crystals with x values close to 0, 0.4, and 0.8 have been investigated. Room-temperature measurements were performed in the five main polarization geometries, including the c-axis polarized configuration. We identify the 4A1g symmetry modes that are Raman allowed within the ideal body-centered-tetragonal unit cell, as well as several disorder activated phonon bands from the BiO and/or SrO layers. For an increasing degree of La doping, the O(2)Sr A1g mode at 624 cm-1 softens by 12 cm-1 between x=0 and x=0.8. We attribute this softening to a weakening of the Cu-O(2)Sr-Bi bond due to a reduction in Cu and Bi valences when going from the overdoped (x=0) to the underdoped (x=0.8) regime.
AB - Phonon Raman spectra of Bi2Sr2-xLaxCuO6+d single crystals with x values close to 0, 0.4, and 0.8 have been investigated. Room-temperature measurements were performed in the five main polarization geometries, including the c-axis polarized configuration. We identify the 4A1g symmetry modes that are Raman allowed within the ideal body-centered-tetragonal unit cell, as well as several disorder activated phonon bands from the BiO and/or SrO layers. For an increasing degree of La doping, the O(2)Sr A1g mode at 624 cm-1 softens by 12 cm-1 between x=0 and x=0.8. We attribute this softening to a weakening of the Cu-O(2)Sr-Bi bond due to a reduction in Cu and Bi valences when going from the overdoped (x=0) to the underdoped (x=0.8) regime.
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M3 - Article
AN - SCOPUS:0008796632
SN - 0163-1829
VL - 56
SP - 2847
EP - 2851
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 5
ER -