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Structural, dynamical and electronic properties of CaCuO2

The scalar relativistic version of an accurate first principles full potential self-consistent linearized muffin tin orbital (LMTO) method has been employed for describing the physical properties of the parent system of the high-T(sub c) oxide superconductors, i.e., CaCuO2. The presently employed modified version of the LMTO method is quite fast and goes beyond the usual LMTO ASA method in the sense that it permits a completely general shape of the potential and the charge density. Also, in contrast to LMTO ASA, the present method is also capable of treating distorted lattice structures accurately. The calculated values of the lattice parameters of pure CaCuO2 lie within 3% of the experimentally measured values for the Sr-doped system Ca(0.86)Sr(0.14)CuO(2). The computed electronic structures and the density of states is quite similar to those of the other oxide superconductors, except of their three- dimensional character because of the presence of strong coupling between the closely spaced CuO2 layers. The van Hove singularity peak appears slightly below the Fermi level and a small concentration of oxygenation /or/ substitutional doping may pin it at the Fermi level. The calculated frequencies for some symmetric frozen phonons for undoped CaCuO2 are quite near to the measured data for the Sr-doped CaCuO2.

Agrawal, Bal K.↗

Materials Data on CaCuO2 by Materials Project

CaCuO2 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Ca2+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Ca–O bond lengths are 2.52 Å. Cu2+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Cu–O bond lengths are 1.94 Å. O2- is bonded to four equivalent Ca2+ and two equivalent Cu2+ atoms to form a mixture of face, edge, and corner-sharing OCa4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–66°.

36 MATERIALS SCIENCE↗

Materials Data on CaCuO2 by Materials Project

CaCuO2 crystallizes in the monoclinic P2_1 space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.42–2.71 Å. In the second Ca2+ site, Ca2+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are a spread of Ca–O bond distances ranging from 2.42–2.72 Å. There are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.94–1.98 Å. In the second Cu2+ site, Cu2+ is bonded in a rectangular see-saw-like geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.94–1.98 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to four Ca2+ and two Cu2+ atoms to form a mixture of corner, edge, and face-sharing OCa4Cu2 octahedra. The corner-sharing octahedral tilt angles are 62°. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Ca2+ and two Cu2+ atoms. In the third O2- site, O2- is bonded to four Ca2+ and two Cu2+ atoms to form a mixture of corner, edge, and face-sharing OCa4Cu2 octahedra. The corner-sharing octahedral tilt angles are 62°. In the fourth O2- site, O2- is bonded in a 6-coordinate geometry to four Ca2+ and two Cu2+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on CaCuO2 by Materials Project

CaCuO2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded to six O2- atoms to form CaO6 octahedra that share corners with two equivalent CaO6 octahedra, a cornercorner with one CuO5 square pyramid, and edges with seven CaO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ca–O bond distances ranging from 2.26–2.51 Å. In the second Ca2+ site, Ca2+ is bonded to six O2- atoms to form CaO6 octahedra that share corners with two equivalent CaO6 octahedra, edges with seven CaO6 octahedra, and edges with two equivalent CuO5 square pyramids. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ca–O bond distances ranging from 2.26–2.51 Å. In the third Ca2+ site, Ca2+ is bonded to six O2- atoms to form CaO6 octahedra that share corners with two equivalent CaO6 octahedra, edges with seven CaO6 octahedra, and edges with two equivalent CuO5 square pyramids. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ca–O bond distances ranging from 2.26–2.47 Å. In the fourth Ca2+ site, Ca2+ is bonded to six O2- atoms to form CaO6 octahedra that share corners with two equivalent CaO6 octahedra, corners with two equivalent CuO5 square pyramids, edges with seven CaO6 octahedra, and an edgeedge with one CuO5 square pyramid. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ca–O bond distances ranging from 2.26–2.47 Å. There are four inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.97–2.04 Å. In the second Cu2+ site, Cu2+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Cu–O bond distances ranging from 1.94–2.78 Å. In the third Cu2+ site, Cu2+ is bonded to five O2- atoms to form distorted CuO5 square pyramids that share corners with three CaO6 octahedra, edges with five CaO6 octahedra, and edges with two equivalent CuO5 square pyramids. The corner-sharing octahedra tilt angles range from 2–15°. There are a spread of Cu–O bond distances ranging from 1.94–2.77 Å. In the fourth Cu2+ site, Cu2+ is bonded in a square co-planar geometry to four O2- atoms. There are a spread of Cu–O bond distances ranging from 1.97–2.04 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded to one Ca2+ and four Cu2+ atoms to form OCaCu4 square pyramids that share corners with seven OCa3Cu2 square pyramids and edges with four OCaCu4 square pyramids. In the second O2- site, O2- is bonded to three Ca2+ and two equivalent Cu2+ atoms to form a mixture of edge and corner-sharing OCa3Cu2 square pyramids. In the third O2- site, O2- is bonded to three Ca2+ and two equivalent Cu2+ atoms to form OCa3Cu2 square pyramids that share corners with five OCaCu4 square pyramids and edges with seven OCa3Cu2 square pyramids. In the fourth O2- site, O2- is bonded to one Ca2+ and four Cu2+ atoms to form a mixture of edge and corner-sharing OCaCu4 square pyramids. In the fifth O2- site, O2- is bonded to three Ca2+ and two equivalent Cu2+ atoms to form a mixture of edge and corner-sharing OCa3Cu2 square pyramids. In the sixth O2- site, O2- is bonded to five Ca2+ and one Cu2+ atom to form distorted OCa5Cu square pyramids that share corners with five OCaCu4 square pyramids and edges with ten OCa3Cu2 square pyramids. In the seventh O2- site, O2- is bonded to three Ca2+ and two equivalent Cu2+ atoms to form a mixture of edge and corner-sharing OCa3Cu2 square pyramids. In the eighth O2- site, O2- is bonded in a 5-coordinate geometry to five Ca2+ and one Cu2+ atom.

36 MATERIALS SCIENCE↗

The series Bi2Sr2Ca(n-1) Cu(n)O(2n+4) (1 less than or equal to n less than or equal to 5): Phase stability and superconducting properties

Phase relations at 850 and 870 C, melting transitions in air, oxygen, and helium were studied for Bi(2.1)Sr(1.9) CuO6 and for the Bi2Sr2Ca(n-1) Cu(n)O(2n+4) for n = 1, 2, 3, 4, 5, and infinity (CaCuO2). Up to 870 C, the n = 2 composition resides in the compatibility tetrahedron bounded by Bi(2+x)(Sr,Ca)(3-y) Cu2O8, (Sr,Ca)14 Cu24O41, Ca2CuO3, and a Bi-Sr-Ca-O phase. The n is greater than or equal to 3 compositions reside in the compatibility tetrahedron Bi(2+x)(Sr,Ca)(3-y) Cu2O8 - (Sr,Ca)14 Cu24O41 - Ca2CuO3 - CuO up to 850 C. However, Bi(2+x)Sr(4-y) Cu3O10 forms for n is greater than or equal to 3 after extended heating at 870 C. Bi(2+x)Sr(2-y) CuO6 and Bi(2+x)(Sr,Ca)(3-y) Cu2O8 melt in air at 914 C and 895 C respectively. During melting, all of the compositions studied lose 1 to 2 percent by weight of oxygen from the reduction of copper. Bi(2+x)Sr(2-y) CuO6, Bi(2+n)(Sr,Ca)(3-y) Cu2O8, and Bi(2+x)(Sr,Ca)(4-y) Cu3O10 exhibit crystallographic alignment in a magnetic field, with the c-axes orienting parallel to the field.

Deguire, Mark R.↗