Abstract
Constant wavelength neutron powder diffraction data at room temperature were used to refine the crystal structures of HgBa2Can-1CunO2n+2+δ (n = 1, 2, 3, 4) superconductors, which were synthesized by solid-state reaction of the component oxides. Samples annealed both in oxygen and argon atmospheres were examined. Rietveld refinements converged to values of Rwp = 8-10% and X2 = 1.1-1.7 using a tetragonal cell with P4/mmm symmetry. The HgBa2CuO4+δ, HgBa2CaCu2O6+δ, and HgBa2Ca2Cu3O8+δ (n = 1, 2, and 3) samples were nearly single phase, whereas the HgBa2Ca3Cu4O10+δ (n = 4) sample was primarily a mixture of the n = 3 and 4 phases. For increasing n, the oxygen-annealed samples exhibit Tc (diamagnetic onsets) of 94, 123, 134, and 124 K, respectively, and a contraction of the CuO2 sheets (lattice parameter a). The highest Tc sample, HgBa2Ca2Cu3O8+δ, has the shortest apical Cu-O bond. Consistently, the atomic displacement parameter for Hg is large. For refinements in which the Hg atomic displacement parameter is fixed at a more reasonable value, occupancies of the Hg site are significantly less than full for the n > 1 samples, suggesting that the Hg site is deficient and/or possibly occupied by atoms with smaller scattering lengths, e.g., Cu. The oxygen site within the Hg layer is partially occupied, and its occupation increases with increasing n. For the argon-annealed samples, the cell volume increases slightly due to the isotropic increase of both the cell parameters and Tc decreases. For HgBa2CaCu2O6+δ, the occupancy of the oxygen site within the Hg layer decreases upon annealing in argon, yet the Tc increased, implying that the initial carrier concentration is in the overdoped regime.
Original language | English |
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Pages (from-to) | 221-230 |
Number of pages | 10 |
Journal | Journal of Solid State Chemistry |
Volume | 122 |
Issue number | 1 |
DOIs | |
State | Published - Feb 15 1996 |
Funding
Thanks are due to Patrick Martin for technical assistance with the a.c. susceptibility measurements. This research was sponsored by the Division of Materials Sciences, Office of Basis Energy Sciences, U.S. Department of Energy and technology development was funded by the U.S. Department of Energy Office of Advanced Utility Concepts-Superconducting Technology Program, both under Contract DE-AC05-84OR21400 with Lockheed-Martin Energy Systems.