The \(1 \mathrm{a}_{2} \mathrm{O}_{3}-\mathrm{CuO}-\mathrm{TiO}_{2}\) system in air at \(960^{\circ} \mathrm{C}\) contains two perovskite-related ternary compounds. \(\mathrm{La}_{2} \mathrm{CuTiO}_{6}\) and \(\left\{\mathrm{La}_{2 / 3} \square_{13} \mathrm{Cu}_{3}\right\}\left(\mathrm{Ti}_{4}\right
The crystal structure of La3Mo4.33Al0.67O14 and the electronic structure of La3Mo4XO14 (X = Si; Mo13Al23; Al12V12)
β Scribed by W.H. McCarroll; K. Podejko; A.K. Cheetham; D.M. Thomas; F.J. DiSalvo
- Publisher
- Elsevier Science
- Year
- 1986
- Tongue
- English
- Weight
- 809 KB
- Volume
- 62
- Category
- Article
- ISSN
- 0022-4596
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A new phase, Bi 13 Mo 4 VO 34 E 13 (E: Bi(III) lone pair) was found in the Bi 2 O 3 -MoO 3 -V 2 O 5 system and its formula determined via single crystal analysis and confirmed by solid state synthesis. It crystallizes in the monoclinic system, space group P2/c, with cell parameters a β«Ψβ¬ 11.652(7) A
## Abstract U~6~Co~23.32~Ge~8~ and U~6~Co~23.5~Si~8~ are prepared by melting of the elements followed by annealing at 1173 K for 14 d.
The principles of X-ray photoelectron spectroscopy are outlined. The application of this technique to the study of the electronic structure of metals, alloy.9 and compounds is illustrated using data in Ag, /3-brass, ReO, and PO,. In the latter a major change in the density of states is observed on p