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Large-shift Raman scattering in insulating parent compounds of cuprate superconductors

Authors
D. SalamonRan LiuM. V. KleinM. A. KarlowS. L. CooperS-W. CheongW. C. LeeD. M. Ginsberg
Issue Date
Mar-1995
Publisher
American Physical Society
Citation
Physical Review B, v.51, no.10, pp 6617 - 6633
Pages
17
Journal Title
Physical Review B
Volume
51
Number
10
Start Page
6617
End Page
6633
URI
https://scholarworks.sookmyung.ac.kr/handle/2020.sw.sookmyung/150887
DOI
10.1103/PhysRevB.51.6617
ISSN
0163-1829
Abstract
We describe the use of large-shift Raman techniques to probe features near the optical conductivity peak in insulating high- T c parent compounds, including the T’-phase materials ( R 2 CuO 4 , R=Gd, Eu, Sm, Nd, Pr), T-phase La 2 CuO 4 , and 123-phase PrBa 2 Cu 3 O 6 and YBa 2 Cu 3 O 6 . We have observed several features near 12 000 cm − 1 (∼1.5 eV) with A 2 g , B 1 g , and A 1 g symmetry. At low temperatures, the largest feature with A 2 g 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 B 1 g feature coinciding in position with the optical conductivity peak is observed in all the T’ phase materials, but not in the other insulators. An A 1 g peak is observed in Gd 2 CuO 4 and Eu 2 CuO 4 40–50 cm − 1 lower in energy than the main A 2 g peak, and in YBa 2 Cu 3 O 6 around 2400 cm − 1 above the main A 2 g 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 d 2 x - y 2 to d x y hole transitions enabled by coupling to oxygen p σ and p π levels.
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