Materials Data on Li2Cu3F11 by Materials Project
Li2Cu3F11 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a distorted trigonal non-coplanar geometry to three F1- atoms. There is two shorter (1.87 Å) and one longer (2.07 Å) Li–F bond length. In the second Li1+ site, Li1+ is bonded in a distorted square co-planar geometry to four F1- atoms. There are two shorter (1.95 Å) and two longer (2.23 Å) Li–F bond lengths. In the third Li1+ site, Li1+ is bonded in a distorted square co-planar geometry to four F1- atoms. There are two shorter (1.94 Å) and two longer (2.23 Å) Li–F bond lengths. In the fourth Li1+ site, Li1+ is bonded in a distorted trigonal non-coplanar geometry to three F1- atoms. There are two shorter (1.88 Å) and one longer (2.13 Å) Li–F bond lengths. There are three inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing CuF6 octahedra. The corner-sharing octahedra tilt angles range from 35–42°. There are a spread of Cu–F bond distances ranging from 1.86–2.01 Å. In the second Cu3+ site, Cu3+ is bonded to six F1- atoms to form corner-sharing CuF6 octahedra. The corner-sharing octahedra tilt angles range from 34–35°. There are a spread of Cu–F bond distances ranging from 1.81–1.94 Å. In the third Cu3+ site, Cu3+ is bonded to six F1- atoms to form a mixture of edge and corner-sharing CuF6 octahedra. The corner-sharing octahedra tilt angles range from 34–44°. There are a spread of Cu–F bond distances ranging from 1.85–2.00 Å. There are fourteen inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Cu3+ atoms. In the second F1- site, F1- is bonded in a distorted bent 120 degrees geometry to one Li1+ and one Cu3+ atom. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Cu3+ atoms. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two equivalent Cu3+ atoms. In the fifth F1- site, F1- is bonded in a bent 150 degrees geometry to two Cu3+ atoms. In the sixth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Cu3+ atoms. In the seventh F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one Cu3+ atom. In the eighth F1- site, F1- is bonded in a bent 150 degrees geometry to two equivalent Cu3+ atoms. In the ninth F1- site, F1- is bonded in a bent 120 degrees geometry to one Li1+ and one Cu3+ atom. In the tenth F1- site, F1- is bonded in a bent 150 degrees geometry to two Cu3+ atoms. In the eleventh F1- site, F1- is bonded in a 3-coordinate geometry to one Li1+ and two equivalent Cu3+ atoms. In the twelfth F1- site, F1- is bonded in a 2-coordinate geometry to two equivalent Cu3+ atoms. In the thirteenth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Li1+ and one Cu3+ atom. In the fourteenth F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two equivalent Cu3+ atoms.
- 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:
- 1732683
- Report Number(s):
- mp-1178131
- Resource Relation:
- Related Information: https://materialsproject.org/citing
- Country of Publication:
- United States
- Language:
- English
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