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Electronic structure studies on the n-type doped superconductors R2−xMxCuO4−δ (R=Pr,Nd,Sm; M=Ce,Th) and Nd2CuO4−xFx by electron-energy-loss spectroscopy

M. Alexander, H. Romberg, N. Nücker, P. Adelmann, J. Fink, J. T. Markert, M. B. Maple, S. Uchida, H. Takagi, Y. Tokura, A. C. W. P. James, D. W. Murphy

DOI 10.1103/PhysRevB.43.333 · Physical Review B

T1

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Abstract

The electronic structure of the high-Tc superconductors R2−xMxCuO4−δ (R=Pr, Nd, Sm; M=Ce, Th) and Nd2CuO3.8F0.2 has been studied by high-energy electron-energy-loss spectroscopy in transmission. Core-level spectroscopy, particularly on O 1s and Cu 2p levels yields information on the partial unoccupied density of states near the Fermi level, while that on R and Ce 3d and 4d levels may serve as a valence monitor for these constituents. A pre-edge structure in the O 1s spectrum is polarized in the CuO2 plane and assigned to transitions into a two-dimensional conduction band consisting of Cu 3d hybridized to O 2p states. In the Cu 3d9 configuration we found a slight admixture (∼10%) of Cu 3d3z2-r2 to the Cu 3dx2-y2 hole states similar to the p-type doped superconductors. Upon doping we recognized a reduction (∼14%) of the excitonic Cu 2p3/2 line, indicating that the introduced electrons go onto the Cu sites, thus producing charge carriers having predominantly Cu 3d character.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Nd1.85Th0.15CuO4-δ

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16Pressure not reportedunknown
Nd1.85Ce0.15CuO4-δ

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23Pressure not reportedunknown
Nd2CuO3.8F0.2

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27Pressure not reportedunknown

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