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Near-band gap electronic structure of the tetragonal rare-earth cuprates R2CuO4 and the bismuth cuprate Bi2CuO4

R. V. Pisarev, V. V. Pavlov, A. M. Kalashnikova, A. S. Moskvin

DOI 10.1103/PhysRevB.82.224502 · Physical Review B

T1

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Abstract

Complex optical dielectric function in the tetragonal rare-earth cuprates R2CuO4 (R=La, Pr, Nd, and Sm) and in the tetragonal bismuth cuprate Bi2CuO4 is studied in the spectral range of 0.6–5.4 eV using a method of optical ellipsometry. The dielectric spectra are studied for the two main polarizations and analyzed in terms of a cluster model for CuO46− complexes taking into account intracenter p−d and intercenter d−d charge-transfer (CT) transitions. The band gap in the rare-earth cuprates is defined by an electric-dipole-allowed CT transitions centered at 1.54–1.59 eV in Pr, Nd, and Sm cuprates, and 2.1 eV in La cuprate. Optical response of Bi2CuO4 strongly differs from the rare-earth cuprates which we relate with strong covalency of Bi-O bonding and strong ionicity of Cu(3d)-O(2p) bonding. These features are manifested in suppression of low-energy intense intracenter p−d and intercenter d−d CT transitions, and by appearance of strong intense absorption bands near 5 eV. Regardless the strong distinctions of optical response, on one hand, of La, Pr, Nd, and Sm cuprates, and on the other hand, of the Bi cuprate, the dielectric gap in these compounds shows comparable values defined by a superposition of intracenter p−d CT transitions and two-center d−d CT transitions. Thus these cuprates should be classified as compounds intermediate between CT and Mott-Hubbard insulators.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
La2CuO4

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—Pressure not reportedunknown
Nd2CuO4

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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