From the studies of the Cu substituted YBa 2 (Cu 1 \_ M )30-\_ (M=Fe, Co, Ni, Zn) systems, it is concluded that the pair-breaking of the AbriRo~ov ~n~Gor'kov type by magnetic impurities is absent, or very small if it exists, both on the C(l) and Cu(2) sites. The Hall coefficient is measured for the
Different origins of Tc-suppression in YBa2(Cu1−xMx)3Oy(M=Co and Zn)
✍ Scribed by Shoji Terada; Norio Kobayashi; Hideo Iwasaki; Ayako Tokiwa; Masae Kikuchi; Yasuhiko Syono; Yoshio Muto
- Publisher
- Elsevier Science
- Year
- 1990
- Tongue
- English
- Weight
- 301 KB
- Volume
- 165-166
- Category
- Article
- ISSN
- 0921-4526
No coin nor oath required. For personal study only.
✦ Synopsis
The electrical resistivity, the Hall effect and the oxygen content have been measured for YBa2(CU 1-xMxhOy(M = Co and Zn). The electrical resistivity increases with concentration x in both systems. The carrier concentration decreases with x for M = Co, while it remains almost constant for M = Zn. The suppression of T e in the Co-doped system is explained by the reduction in carrier. In the Zn-doped system, on the other hand, the suppression seems to be caused by the electron localization in Cu-O planes. K)()
200 JOO
Tl'mpE'ralure ( K)
📜 SIMILAR VOLUMES
We report here on the changes in behavior, including transitions from superconducting to semiconducting, as a function of heat treatment of YBa2 (Cu~\_xNix) 3Oy with x = 0.05. In particular, conventional materials prepared by slow cooling from ~ 1200 K (designated OP for oxygenating preparations), s
We present structural, magnetic and superconducting properties of conventionally, and reductively prepared equilibrium states of YBa,(Cu,\_,M,)sO, with M = Fe, Co, Ni. Depending on preparation conditions, varying clustering tendencies for M on Cu(l) are found. A highly ordered cluster state :U) mani
YBa2 ( Cu ~ \_ xMx ) 4Os ( M = Fe, Co, Ni, Zn and Ga; 0 ~< x ~< 0.05 ) h ave been investigated by means of X-ray diffraction, electrical-resistivity and magnetic-susceptibility measurements. X-ray-diffraction patterns show that all samples studied contain the nearly single 124 phase. They exhibit an
We performed an analysis for fine structure of Gd ESR spectra near 4K on Gdo.o5Yo.95Ba2(CUl\_ x M )^O , to study the interaction between Gd and their environment. From the analysis, we obtain the • x 3.y crystalline field parameter, D, and Gd spin suseptibility, /spin" Hagnetic properties of our sy