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Materials Data on Sr2Cu3O5 by Materials Project

Sr2Cu3O5 crystallizes in the orthorhombic Cmmm space group. The structure is three-dimensional. Sr2+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are six shorter (2.64 Å) and two longer (2.66 Å) Sr–O bond lengths. There are two 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 1.91–1.97 Å. In the second Cu2+ site, Cu2+ is bonded in a square co-planar geometry to four O2- atoms. There is two shorter (1.97 Å) and two longer (1.99 Å) Cu–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Sr2+ and three equivalent Cu2+ atoms to form distorted OSr2Cu3 trigonal bipyramids that share corners with seven OSr4Cu2 octahedra, corners with four equivalent OSr2Cu3 trigonal bipyramids, an edgeedge with one OSr4Cu2 octahedra, edges with two equivalent OSr2Cu3 trigonal bipyramids, and faces with two equivalent OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–64°. In the second O2- site, O2- is bonded to four equivalent Sr2+ and two Cu2+ atoms to form distorted OSr4Cu2 octahedra that share corners with nine OSr4Cu2 octahedra, corners with five equivalent OSr2Cu3 trigonal bipyramids, edges with four equivalent OSr4Cu2 octahedra, faces with two equivalent OSr4Cu2 octahedra, and faces with two equivalent OSr2Cu3 trigonal bipyramids. The corner-sharing octahedra tilt angles range from 0–64°. In the third O2- site, O2- is bonded to four equivalent Sr2+ and two equivalent Cu2+ atoms to form OSr4Cu2 octahedra that share corners with ten OSr4Cu2 octahedra, corners with four equivalent OSr2Cu3 trigonal bipyramids, edges with two equivalent OSr4Cu2 octahedra, edges with two equivalent OSr2Cu3 trigonal bipyramids, and faces with four equivalent OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–64°.

36 MATERIALS SCIENCE↗

Materials Data on Sr2Cu3O5 by Materials Project

Sr2Cu3O5 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. Sr2+ is bonded in a body-centered cubic geometry to eight O2- atoms. There are six shorter (2.63 Å) and two longer (2.74 Å) Sr–O bond lengths. There are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded in a square co-planar geometry to four O2- atoms. There is two shorter (1.94 Å) and two longer (1.98 Å) Cu–O bond length. In the second Cu2+ site, Cu2+ is bonded to five O2- atoms to form a mixture of edge and corner-sharing CuO5 trigonal bipyramids. There are a spread of Cu–O bond distances ranging from 1.98–2.16 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Sr2+ and two Cu2+ atoms to form a mixture of edge, face, and corner-sharing OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–65°. In the second O2- site, O2- is bonded to four equivalent Sr2+ and two equivalent Cu2+ atoms to form a mixture of edge, face, and corner-sharing OSr4Cu2 octahedra. The corner-sharing octahedra tilt angles range from 0–65°. In the third O2- site, O2- is bonded to two equivalent Sr2+ and four equivalent Cu2+ atoms to form a mixture of distorted edge, face, and corner-sharing OSr2Cu4 octahedra. The corner-sharing octahedra tilt angles range from 2–65°.

36 MATERIALS SCIENCE↗

High pressure synthesis and magnetic studies of quasi one dimensional systems Sr(n-1)Cu(n+1)O(2n) (n=3,5)

SrCu2O3 and Sr2Cu3O5 containing two-leg and three-leg S = 1/2 ladders made of antiferromagnetic Cu-O-Cu linear bonds, respectively, were synthesized at high pressure, and their crystallographic and magnetic properties were investigated. Both susceptibility and T(1) data of NMR (nuclear magnetic resonance) revealed the existence of a large spin gap only for SrCu2O3. Superconductivity, which had been predicted theoretically for carrier-doped SrCu2O3 could not be realized although partial substitution of La(3+) for Sr(2+) seemed to be carried out successfully. Electron carriers injected seems to remain localized.

Azuma, M.↗