Single crystals of Ag 2 Cu 2 O 3 were prepared by solid state reaction of Ag 2 O and CuO applying an oxygen pressure of 200 MPa. Crystals of Ag 2 Cu 2 O 3 (I4 1 /amd, a โซุโฌ 589.78(6), c โซุโฌ 1071.4( 2) pm from single crystal data, Z โซุโฌ 4, 289 unique di4ractometer data, R1 โซุโฌ 0.043, wR2 โซุโฌ 0.098) a
Description of the ground state electronic structures of Cu2O, Cu2S, Ag2O and Ag2S
โ Scribed by David A. Dixon; James L. Gole
- Publisher
- Elsevier Science
- Year
- 1992
- Tongue
- English
- Weight
- 435 KB
- Volume
- 189
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
The electronic structures of the copper and silver oxides CuaO, Cu*S, Ag,O and Ag,S have been calculated in the local density functional approximation.
The structures closely resemble an O-or S-bridging an M $ as shown by the geometries and the charge distributions.
The symmetric stretch frequency exceeds that of the asymmetric stretch as well as the stretch in the free diatomic. The electronic structures of the oxides and sulfides are similar with the HOMO having most of its density on the oxygen or sulfur. The predicted ionization potentials are also similar.
๐ SIMILAR VOLUMES
Extended basis set calculations have been performed for the ground state of 0.12 using CI(SD) and the coupled pair functional (CPF) method, a size-consistent moditication of CI(SD). Special emphasis is ,&en to the discussion of (lj Scis saturation effects (up to g functions were included). a) effect
in their 'C,' ground states have been observed in solid neon matrices at 4 K via X-band electron-spinresonance (ESR) spectroscopy. The g and hyperfine tensor components of each cation have been interpreted in terms of the orbital characteristics of the unpaired electron.
The electronic structure of the ground state and the doublet excited states due to 3d ยช 3d transitions and charge-transfer transitions from ligand to copper of ลฝ . 2 q Cu H O are investigated by ab initio calculations. The excited states corresponding to 2 6 the 3d ยช 3d transitions are calculated to