STRUCTURE, SUPERCONDUCTIVITY AND MAGNETISM OF YBA2(CU(1-X)M(X))(4)O-8(M=FE, CO, NI, ZN AND GA)

Citation
Th. Meen et al., STRUCTURE, SUPERCONDUCTIVITY AND MAGNETISM OF YBA2(CU(1-X)M(X))(4)O-8(M=FE, CO, NI, ZN AND GA), Physica. C, Superconductivity, 242(3-4), 1995, pp. 373-380
Citations number
32
Categorie Soggetti
Physics, Applied
ISSN journal
09214534
Volume
242
Issue
3-4
Year of publication
1995
Pages
373 - 380
Database
ISI
SICI code
0921-4534(1995)242:3-4<373:SSAMOY>2.0.ZU;2-J
Abstract
YBa2(Cu(1-x)M(x))(4)O-8 (M=Fe, Co, Ni, Zn and Ga; 0 less than or equal to x less than or equal to 0.05) have been investigated by means of X -ray diffraction, electrical-resistivity and magnetic-susceptibility m easurements. X-ray-diffraction patterns show that all samples studied contain the nearly single 124 phase. They exhibit an orthorhombio-to-t etragonal structural transition at about x=0.03 for M=Fe and Co; and a t x=0.04 for M=Ga; while the structure remains orthorhombic at x=0.05 for M=Ni and Zn. These results suggest that Fe, Co and Ga substitute p referentially for [Cu(1)] sites, and the Ni and Zn prefer to occupy th e [Cu(2)] sites. The initial depression rates of T-c0 (temperature of zero resistance) with increasing doping concentration for various dopa nts are 16.85, 8.4, 23.75, 12 and 3.9 K/at.% for M=Fe, Co, Ni, Zn and Ga, respectively. Effective magnetic moments of YBa2(Cu(0.97)M(0.03))( 4)O-8 are 5.63, 3.91 and 3.37 mu(B) for M=Fe, Co and Ni, respectively. In addition, the similarities and differences between YBa2(Cu(1-x)M(x ))(4)O-8 and YBa2(Cu(1-x)M(x))(3)O-7-y are discussed.