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
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
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
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| La2CuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nd2CuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Generalized cuprate gap symmetry and higher d-wave harmonics: Effects of correlation length, doping, temperature, and impurity scattering
similarity 0.94David Parker et al.
Source status unknown — claims are unverified
High-energy spin excitations in the insulating phases of high-Tc superconducting cuprates and La2NiO4
similarity 0.94S. Sugai et al.
Source status unknown — claims are unverified
Asymmetry of superconductivity in hole- and electron-doped cuprates: Explanation within two-particle self-consistent analysis for the three-band model
similarity 0.94Daisuke Ogura & Kazuhiko Kuroki
Source status unknown — claims are unverified
Tuning the in-plane electron behavior in high-Tc cuprate superconductors via apical atoms: A first-principles Wannier-states analysis
similarity 0.94Wei-Guo Yin & Wei Ku
Source status unknown — claims are unverified
Theoretical study of the structural dependence of nuclear quadrupole frequencies in high-Tc superconductors
similarity 0.94M. E. Garcia & K. H. Bennemann
Source status unknown — claims are unverified
Theoretical Demonstration of How the Dispersion of Magnetic Excitations in Cuprate Compounds can be Determined Using Resonant Inelastic X-Ray Scattering
similarity 0.93Luuk J. P. Ament et al.
Source status unknown — claims are unverified