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Three phases in the system Hg{sub 1{minus}x}C{sub x}Ba{sub 2}CuO{sub y} (0.00 {le} x {le} 1.00)

Journal Article · · Materials Research Bulletin
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  1. CNRS-UJF, Grenoble (France). Lab. de Cristallographie
Samples of the [Hg{sub 1{minus}x}C{sub x}]-Ba{sub 2}CuO{sub y} system [(Hg,C)-1201] with stoichiometries within the range 0.00 {le} x {le} 1.00 were synthesized by a high-pressure, high-temperature technique. The sample with x = 0.00 [HgBa{sub 2}CuO{sub 4+{delta}}] was non-superconducting with lattice parameters a = 3,8676(2) {angstrom}, c = 9.470(1) {angstrom}. At low ranges of substitution (0.10 {le} x {le} 0.30), the predominant phase was found to be Hg-1201 with identical lattice parameters to those found for x = 0.00. At x = 0.40 the Hg-1201 phase coexists in similar proportions with the phase of mixed [Hg{sub 1{minus}x}, C{sub x}]-1201 stoichiometry. At x = 0.50, this second phase with lattice parameters a = 3.9271(3) {angstrom}, c = 8.676(2) {angstrom} is predominant and only traces of the Hg-1201 phase were found. At x = 0.75 the [Hg{sub 1{minus}x}, C{sub x}]-1201 phase found for x = 0.50 coexists with the CO{sub 3}Ba{sub 2}CuO{sub y} phase, which is the extreme of the substitution range. This latter was predominant at x = 1.00 with lattice parameters a = 4.0044(3) {angstrom}, c = 7.909(1) {angstrom}, but at higher pressure than the previous substitutions. This system is constituted of three main phases, HgBa{sub 2}CuO{sub 4+{delta}}, Hg{sub 1{minus}x}C{sub x}Ba{sub 2}CuO{sub y} (x {approx} 0.50) and CO{sub 3}Ba{sub 2}CuO{sub y}, which appear in different proportions according to the percentage of substitution and the applied synthesis pressure.
OSTI ID:
175859
Journal Information:
Materials Research Bulletin, Journal Name: Materials Research Bulletin Journal Issue: 12 Vol. 30; ISSN MRBUAC; ISSN 0025-5408
Country of Publication:
United States
Language:
English