Coexistence curves of (T, n), (T, x), and (T, φ) where n, x, and φ are the refractive index, the mole fraction, and the volume fraction, respectively, for the binary mixtures {xC 6 H 5 NO 2 +(1x)CH 3 (CH 2 ) 4 CH 3 } and {xC 6 H 5 NO 2 +(1x)CH 3 (CH 2 ) 5 CH 3 } have been determined within about 10
Coexistence of magnetism and superconductivity in R1.4Ce0.6RuSr2Cu2O10 − δ(R = Eu, Sm and Gd)
✍ Scribed by I. Felner; U. Asaf
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 109 KB
- Volume
- 24
- Category
- Article
- ISSN
- 0749-6036
No coin nor oath required. For personal study only.
✦ Synopsis
The superconducting R 1.4 Ce 0.6 RuSr 2 Cu 2 O 10-δ (R = Sm, Eu and Gd) with T c ∼ 28, 32 and 42 K are also magnetically ordered at T N ∼ 220, 122 and 180 K, respectively, thus, T N T c . This is in contrast to intermetallic magnetic superconductors (such as RNi 2 B 2 C) in which T c > T N . Magnetic susceptibility and Mossbauer spectroscopy show that superconductivity is confined to the CuO 2 planes, whereas magnetism is due to the Ru sublattice. Irreversibility phenomena and magnetic anomalies, observed at low magnetic fields originate from antisymmetric exchange coupling of the Dzyaloshinsky-Moria type, and from spin reorientation of the Ru moments. The shielding fraction is about 100%, supporting the conclusion that the materials consist of a single phase, manifesting both magnetism and superconductivity at once.
📜 SIMILAR VOLUMES
HgBa 2 CuO 4+δ and (Ca x La 1-x )(Ba 1.75-x La 0.25+x )Cu 3 O 7±δ superconducting systems were structurally investigated employing Rietveld analysis. The doping of holes in Hg compounds was done by oxygenation and reduction methods. In Ca-La-Ba-Cu-O system the doping of holes was introduced via cati