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Materials Data on CsLiBr2 by Materials Project

CsLiBr2 crystallizes in the tetragonal P4/nmm space group. The structure is three-dimensional. Cs1+ is bonded in a 5-coordinate geometry to nine Br1- atoms. There are a spread of Cs–Br bond distances ranging from 3.69–4.03 Å. Li1+ is bonded to five Br1- atoms to form a mixture of distorted edge and corner-sharing LiBr5 trigonal bipyramids. There are one shorter (2.53 Å) and four longer (2.75 Å) Li–Br bond lengths. There are two inequivalent Br1- sites. In the first Br1- site, Br1- is bonded to five equivalent Cs1+ and one Li1+ atom to form a mixture of distorted edge and corner-sharing BrCs5Li octahedra. The corner-sharing octahedral tilt angles are 10°. In the second Br1- site, Br1- is bonded in a 4-coordinate geometry to four equivalent Cs1+ and four equivalent Li1+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Cs3Li2Br5 by Materials Project

Cs3Li2Br5 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are two inequivalent Cs1+ sites. In the first Cs1+ site, Cs1+ is bonded in a body-centered cubic geometry to eight Br1- atoms. There are a spread of Cs–Br bond distances ranging from 3.72–3.93 Å. In the second Cs1+ site, Cs1+ is bonded in a body-centered cubic geometry to eight Br1- atoms. There are a spread of Cs–Br bond distances ranging from 3.75–3.85 Å. Li1+ is bonded to four Br1- atoms to form corner-sharing LiBr4 tetrahedra. There are a spread of Li–Br bond distances ranging from 2.52–2.60 Å. There are three inequivalent Br1- sites. In the first Br1- site, Br1- is bonded in a body-centered cubic geometry to eight Cs1+ atoms. In the second Br1- site, Br1- is bonded in a distorted trigonal non-coplanar geometry to two equivalent Cs1+ and three equivalent Li1+ atoms. In the third Br1- site, Br1- is bonded in a distorted single-bond geometry to six Cs1+ and one Li1+ atom.

36 MATERIALS SCIENCE↗