𝔖 Bobbio Scriptorium
✦   LIBER   ✦

The nature and the role of rock salt-type layers in superconductive layered copper oxides

✍ Scribed by B. Raveau; C. Michel; J. Provost; M. Hervieu

Publisher
Elsevier Science
Year
1990
Tongue
English
Weight
305 KB
Volume
40-41
Category
Article
ISSN
0167-2738

No coin nor oath required. For personal study only.

πŸ“œ SIMILAR VOLUMES

The Great Flexibility of the Rock Salt L
The Great Flexibility of the Rock Salt Layers in the Lead-Based 1212 High-Tc Superconductive Cuprates: The Oxides (Pb, A)Sr2(Ca, Ln)Cu2O7-Ξ΄
✍ A. Maignan; D. Groult; R.S. Liu; T. Rouillon; P. Daniel; C. Michel; M. Hervieu; πŸ“‚ Article πŸ“… 1993 πŸ› Elsevier Science 🌐 English βš– 293 KB

A systematic investigation of superconductivity based on 1212-type cuprates with nominal compositions \(\left(\mathrm{Pb}_{0.5} A_{0.5}\right) \mathrm{Sr}_{2}\left(\mathrm{Ca}_{0.5} \mathrm{Y}_{0.5}\right) \mathrm{Cu}_{2} \mathrm{O}_{7 . \delta}\) with \(A=\mathrm{Cu}, \mathrm{Zn}, \mathrm{Ni}, \mat

The labile magnetic structure of JT copp
The labile magnetic structure of JT copper and nickel complexes in the layered oxides
✍ Yu.V. Yablokov; T.A. Ivanova πŸ“‚ Article πŸ“… 1999 πŸ› Elsevier Science 🌐 English βš– 177 KB

The structure and dynamics of magnetic centers and magnetic structures in oxides of A 2 BO 4 type are considered. The local and cooperative Jahn -Teller effect and the lattice perturbations are shown to determine the character of distortions of MeO 6 complexes (Me =Cu 2 + , Ni 3 + ) in LaSrAl 1 -x M

The important role of pyramidal copper l
The important role of pyramidal copper layers of the 123-structure in superconductivity: The oxides Ba2Y1βˆ’xCaxCu3βˆ’xFexO7 and Ba2Y1βˆ’xCaxCu3βˆ’xFexO6
✍ E. Suard; V. Caignaert; A. Maignan; B. Raveau πŸ“‚ Article πŸ“… 1991 πŸ› Elsevier Science 🌐 English βš– 665 KB

Three series of oxides Ba,Y, \_,CaXCu3\_,FeX0,, tetragonal and orthorhombic, and Ba,Y I \_XCaXCu,\_,FeXO, tetragonal, have been synthesized by successive appropriate thermal treatments under oxygen and argon, for x=0.09,0.12,0.15,0.24. The structure of these different forms has been determined by ne