TY - JOUR
T1 - Large-shift Raman scattering in insulating parent compounds of cuprate superconductors
AU - Salamon, D.
AU - Liu, Ran
AU - Klein, M. V.
AU - Karlow, M. A.
AU - Cooper, S. L.
AU - Cheong, S. W.
AU - Lee, W. C.
AU - Ginsberg, D. M.
PY - 1995
Y1 - 1995
N2 - We describe the use of large-shift Raman techniques to probe features near the optical conductivity peak in insulating high-Tc parent compounds, including the T'-phase materials (R2CuO4, R=Gd, Eu, Sm, Nd, Pr), T-phase La2CuO4, and 123-phase PrBa2Cu3O6 and YBa2Cu3O6. We have observed several features near 12 000 cm-1 (∼1.5 eV) with A2g, B1g, and A1g symmetry. At low temperatures, the largest feature with A2g symmetry splits in all the insulating cuprates into three distinct peaks: a strong main peak, and two weaker sidebands offset approximately 600 and 1500 cm-1 higher in energy, respectively. A B1g feature coinciding in position with the optical conductivity peak is observed in all the T' phase materials, but not in the other insulators. An A1g peak is observed in Gd2CuO4 and Eu2CuO4 40-50 cm-1 lower in energy than the main A2g peak, and in YBa2Cu3O6 around 2400 cm-1 above the main A2g peak. All of these features have unusual, temperature-dependent resonance behavior with the incident photon energy. We propose explanations for many of the above observations involving copper dx2-y2 to dxy hole transitions enabled by coupling to oxygen pσ and pπ levels.
AB - We describe the use of large-shift Raman techniques to probe features near the optical conductivity peak in insulating high-Tc parent compounds, including the T'-phase materials (R2CuO4, R=Gd, Eu, Sm, Nd, Pr), T-phase La2CuO4, and 123-phase PrBa2Cu3O6 and YBa2Cu3O6. We have observed several features near 12 000 cm-1 (∼1.5 eV) with A2g, B1g, and A1g symmetry. At low temperatures, the largest feature with A2g symmetry splits in all the insulating cuprates into three distinct peaks: a strong main peak, and two weaker sidebands offset approximately 600 and 1500 cm-1 higher in energy, respectively. A B1g feature coinciding in position with the optical conductivity peak is observed in all the T' phase materials, but not in the other insulators. An A1g peak is observed in Gd2CuO4 and Eu2CuO4 40-50 cm-1 lower in energy than the main A2g peak, and in YBa2Cu3O6 around 2400 cm-1 above the main A2g peak. All of these features have unusual, temperature-dependent resonance behavior with the incident photon energy. We propose explanations for many of the above observations involving copper dx2-y2 to dxy hole transitions enabled by coupling to oxygen pσ and pπ levels.
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U2 - 10.1103/PhysRevB.51.6617
DO - 10.1103/PhysRevB.51.6617
M3 - Article
AN - SCOPUS:0001372356
SN - 0163-1829
VL - 51
SP - 6617
EP - 6633
JO - Physical Review B
JF - Physical Review B
IS - 10
ER -