Nr. Khasanova et al., CRYSTAL-STRUCTURE OF THE SUPERCONDUCTOR CA2SR2CU3GAO9 SYNTHESIZED AT HIGH-PRESSURE, Physica. C, Superconductivity, 258(3-4), 1996, pp. 227-235
Ca2Sr2Cu3GaO9 with a T-c of 73 K was prepared at 1250 degrees C and 6
GPa. Its neutron powder diffraction data were analyzed on the basis of
Ima2, Imcm and P2(1)ab space groups. Imcm gave the best approximation
to the actual superstructure with a doubled b dimension. Ca2Sr2Cu3GaO
9 belongs to a homologous series of oxides (R(1-x)Ca(x))(n-1)Sr2CunGaO
2n+3 (R: rare-earth metals). In its structure, GaO4 tetrahedra form (G
aO33-)(x) chains running parallel with the c-axis. Sr2GaO3 blocks comp
osed of the infinite chains and Sr2+ ions alternate with (Ca)(2)(CuO2)
(3) sheets along the a-axis. Two types of the infinite chains with dif
ferent orientations of GaO4 tetrahedra alternate along the b-axis, whi
ch is the reason for the 2b superstructure. The Cu(1)O-5 pyramid tilts
owing to the tetrahedral coordination of Ga. The intermediate Cu(2)O-
2 sheet is nearly flat with each Cu(2) atom having four equivalent Cu-
O bonds. Sr2+ and Ca2+ ions are completely ordered on two different si
tes. Full occupation of Ca2+ ions at an eight-coordinated site, which
is obtained only at high pressure, permits adequate hole doping of the
CuO2 sheets, where the formal oxidation state of Cu is +2.33.