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Title: Materials Data on Ba2CaTl2(CuO3)4 by Materials Project

Dataset ·
DOI:https://doi.org/10.17188/1318342· OSTI ID:1318342

Ca(CuO2)2(BaCuTlO4)2 crystallizes in the tetragonal I4/mmm space group. The structure is two-dimensional and consists of two BaCuTlO4 sheets oriented in the (0, 0, 1) direction and two Ca(CuO2)2 sheets oriented in the (0, 0, 1) direction. In each BaCuTlO4 sheet, Ba2+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are four shorter (2.69 Å) and four longer (2.85 Å) Ba–O bond lengths. Cu3+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Cu–O bond lengths are 1.92 Å. Tl3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are one shorter (2.09 Å) and four longer (2.25 Å) Tl–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to four equivalent Ba2+ and one Tl3+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+ and two equivalent Cu3+ atoms. In the third O2- site, O2- is bonded to four equivalent Tl3+ atoms to form a mixture of edge and corner-sharing OTl4 tetrahedra. In each Ca(CuO2)2 sheet, Ca2+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Ca–O bond lengths are 2.41 Å. Cu3+ is bonded in a square co-planar geometry to four equivalent O2- atoms. All Cu–O bond lengths are 1.92 Å. O2- is bonded to two equivalent Ca2+ and two equivalent Cu3+ atoms to form a mixture of distorted edge and corner-sharing OCa2Cu2 trigonal pyramids.

Research Organization:
Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States). LBNL Materials Project
Sponsoring Organization:
USDOE Office of Science (SC), Basic Energy Sciences (BES)
Contributing Organization:
MIT; UC Berkeley; Duke; U Louvain
DOE Contract Number:
AC02-05CH11231; EDCBEE
OSTI ID:
1318342
Report Number(s):
mvc-11852
Resource Relation:
Related Information: https://materialsproject.org/citing
Country of Publication:
United States
Language:
English

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