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Title: Materials Data on Li2CuF5 by Materials Project

Abstract

Li2CuF5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with three CuF6 octahedra, an edgeedge with one LiF6 octahedra, and edges with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 49–58°. There are a spread of Li–F bond distances ranging from 1.92–2.34 Å. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.87–2.33 Å. There are two inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded to six F1- atoms to form CuF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with two equivalent CuF6 octahedra, and edges with four equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 49–55°. There are a spread of Cu–F bond distances ranging from 1.90–1.99 Å. In the second Cu3+ site, Cu3+ is bonded to six F1- atoms to form CuF6 octahedra that share corners with two equivalent CuF6 octahedra and corners with fourmore » equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 50–58°. There are a spread of Cu–F bond distances ranging from 1.79–2.34 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom. In the second F1- site, F1- is bonded to three Li1+ and one Cu3+ atom to form a mixture of distorted edge and corner-sharing FLi3Cu trigonal pyramids. In the third F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ and one Cu3+ atom. In the fourth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two Cu3+ atoms. In the fifth F1- site, F1- is bonded in a trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom.« less

Publication Date:
Other Number(s):
mp-781976
DOE Contract Number:  
AC02-05CH11231
Research Org.:
LBNL Materials Project; Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22)
Collaborations:
The Materials Project; MIT; UC Berkeley; Duke; U Louvain
Subject:
36 MATERIALS SCIENCE; Cu-F-Li; Li2CuF5; crystal structure
OSTI Identifier:
1307605
DOI:
https://doi.org/10.17188/1307605

Citation Formats

Materials Data on Li2CuF5 by Materials Project. United States: N. p., 2020. Web. doi:10.17188/1307605.
Materials Data on Li2CuF5 by Materials Project. United States. doi:https://doi.org/10.17188/1307605
2020. "Materials Data on Li2CuF5 by Materials Project". United States. doi:https://doi.org/10.17188/1307605. https://www.osti.gov/servlets/purl/1307605. Pub date:Sat May 02 00:00:00 EDT 2020
@article{osti_1307605,
title = {Materials Data on Li2CuF5 by Materials Project},
abstractNote = {Li2CuF5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six F1- atoms to form distorted LiF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with three CuF6 octahedra, an edgeedge with one LiF6 octahedra, and edges with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 49–58°. There are a spread of Li–F bond distances ranging from 1.92–2.34 Å. In the second Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five F1- atoms. There are a spread of Li–F bond distances ranging from 1.87–2.33 Å. There are two inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded to six F1- atoms to form CuF6 octahedra that share corners with two equivalent LiF6 octahedra, corners with two equivalent CuF6 octahedra, and edges with four equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 49–55°. There are a spread of Cu–F bond distances ranging from 1.90–1.99 Å. In the second Cu3+ site, Cu3+ is bonded to six F1- atoms to form CuF6 octahedra that share corners with two equivalent CuF6 octahedra and corners with four equivalent LiF6 octahedra. The corner-sharing octahedra tilt angles range from 50–58°. There are a spread of Cu–F bond distances ranging from 1.79–2.34 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom. In the second F1- site, F1- is bonded to three Li1+ and one Cu3+ atom to form a mixture of distorted edge and corner-sharing FLi3Cu trigonal pyramids. In the third F1- site, F1- is bonded in a 1-coordinate geometry to two Li1+ and one Cu3+ atom. In the fourth F1- site, F1- is bonded in a 4-coordinate geometry to two Li1+ and two Cu3+ atoms. In the fifth F1- site, F1- is bonded in a trigonal planar geometry to two equivalent Li1+ and one Cu3+ atom.},
doi = {10.17188/1307605},
journal = {},
number = ,
volume = ,
place = {United States},
year = {2020},
month = {5}
}