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(Cs)2SiP2 crystallizes in the orthorhombic Ibam space group. The structure is one-dimensional and consists of eight cesium molecules and two SiP2 ribbons oriented in the (1, 0, 0) direction. In each SiP2 ribbon, Si4- is bonded in a 4-coordinate geometry to four equivalent P1+ atoms. All Si–P bond lengths are 2.30 Å. P1+ is bonded in an L-shaped geometry to two equivalent Si4- atoms.
(Cs)2CsYI6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsYI6 framework. In the CsYI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent YI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.64 Å. Y3+ is bonded to six equivalent I1- atoms to form YI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Y–I bond lengths are 3.03 Å. I1- is bonded in a linear geometry to one Cs1+ and one Y3+ atom.
(Cs)2RbBiI6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one RbBiI6 framework. In the RbBiI6 framework, Rb1+ is bonded to six equivalent I1- atoms to form RbI6 octahedra that share corners with six equivalent BiI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Rb–I bond lengths are 3.50 Å. Bi3+ is bonded to six equivalent I1- atoms to form BiI6 octahedra that share corners with six equivalent RbI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Bi–I bond lengths are 3.08 Å. I1- is bonded in a linear geometry to one Rb1+ and one Bi3+ atom.
(Cs)2CsInI6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsInI6 framework. In the CsInI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent InI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.62 Å. In3+ is bonded to six equivalent I1- atoms to form InI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All In–I bond lengths are 2.95 Å. I1- is bonded in a linear geometry to one Cs1+ and one In3+ atom.
(Cs)2CsBiI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsBiI6 framework. In the CsBiI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent BiI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.63 Å. Bi3+ is bonded to six equivalent I1- atoms to form BiI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Bi–I bond lengths are 3.09 Å. I1- is bonded in a linear geometry to one Cs1+ and one Bi3+ atom.
Cs is alpha structured and crystallizes in the cubic I-43m space group. The structure is three-dimensional and consists of two cesium molecules and one Cs framework. In the Cs framework, there are three inequivalent Cs sites. In the first Cs site, Cs is bonded in a trigonal non-coplanar geometry to three equivalent Cs atoms. All Cs–Cs bond lengths are 5.32 Å. In the second Cs site, Cs is bonded in a 8-coordinate geometry to eight Cs atoms. There are a spread of Cs–Cs bond distances ranging from 4.90–5.56 Å. In the third Cs site, Cs is bonded in a 8-coordinate geometry to eight Cs atoms. Both Cs–Cs bond lengths are 5.52 Å.
CsSiI3 is Pb (Zr_0.50 Ti_0.48) O_3 structured and crystallizes in the triclinic P1 space group. The structure is zero-dimensional and consists of one cesium molecule and one triiodosilane molecule.
CsCs6NaSi8 crystallizes in the cubic Pa-3 space group. The structure is three-dimensional and consists of four cesium molecules and one Cs6NaSi8 framework. In the Cs6NaSi8 framework, Cs1+ is bonded in a 6-coordinate geometry to six Si1- atoms. There are a spread of Cs–Si bond distances ranging from 3.67–3.95 Å. Na1+ is bonded in a 6-coordinate geometry to six equivalent Si1- atoms. All Na–Si bond lengths are 3.00 Å. There are two inequivalent Si1- sites. In the first Si1- site, Si1- is bonded in a 9-coordinate geometry to six equivalent Cs1+ and three equivalent Si1- atoms. All Si–Si bond lengths are 2.42 Å. In the second Si1- site, Si1- is bonded in a 1-coordinate geometry to four equivalent Cs1+, one Na1+, and three Si1- atoms. Both Si–Si bond lengths are 2.47 Å.
CsAuC2 crystallizes in the tetragonal P4/mmm space group. The structure is one-dimensional and consists of one cesium molecule and one AuC2 ribbon oriented in the (0, 0, 1) direction. In the AuC2 ribbon, Au1- is bonded in a linear geometry to two equivalent C atoms. Both Au–C bond lengths are 2.00 Å. C is bonded in a linear geometry to one Au1- and one C atom. The C–C bond length is 1.25 Å.
(Cs)3Hg is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is zero-dimensional and consists of three cesium molecules and one mercury molecule.
(Cs)2CsBiBr6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsBiBr6 framework. In the CsBiBr6 framework, Cs1+ is bonded to six equivalent Br1- atoms to form CsBr6 octahedra that share corners with six equivalent BiBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Br bond lengths are 3.42 Å. Bi3+ is bonded to six equivalent Br1- atoms to form BiBr6 octahedra that share corners with six equivalent CsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Bi–Br bond lengths are 2.87 Å. Br1- is bonded in a linear geometry to one Cs1+ and one Bi3+ atom.
CsK2As is Cyanogen Chloride-like structured and crystallizes in the orthorhombic Immm space group. The structure is zero-dimensional and consists of two cesium molecules and two K2As clusters. In each K2As cluster, K1+ is bonded in a single-bond geometry to one As3- atom. The K–As bond length is 3.13 Å. As3- is bonded in a linear geometry to two equivalent K1+ atoms.
(Cs)2CsTlI6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsTlI6 framework. In the CsTlI6 framework, Cs1+ is bonded to six equivalent I1- atoms to form CsI6 octahedra that share corners with six equivalent TlI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–I bond lengths are 3.61 Å. Tl3+ is bonded to six equivalent I1- atoms to form TlI6 octahedra that share corners with six equivalent CsI6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Tl–I bond lengths are 3.02 Å. I1- is bonded in a linear geometry to one Cs1+ and one Tl3+ atom.
RbCs2Sb is Cyanogen Chloride-like structured and crystallizes in the orthorhombic Immm space group. The structure is zero-dimensional and consists of two antimony;cesium molecules and two rubidium molecules.
Cs3LaCl6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsLaCl6 framework. In the CsLaCl6 framework, Cs1+ is bonded to six equivalent Cl1- atoms to form CsCl6 octahedra that share corners with six equivalent LaCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Cl bond lengths are 3.29 Å. La3+ is bonded to six equivalent Cl1- atoms to form LaCl6 octahedra that share corners with six equivalent CsCl6 octahedra. The corner-sharing octahedral tilt angles are 0°. All La–Cl bond lengths are 2.78 Å. Cl1- is bonded in a linear geometry to one Cs1+ and one La3+ atom.
CsNbC6 crystallizes in the cubic Pm-3m space group. The structure is three-dimensional and consists of one cesium molecule and one NbC6 framework. In the NbC6 framework, Nb5+ is bonded in an octahedral geometry to six equivalent C1- atoms. All Nb–C bond lengths are 2.18 Å. C1- is bonded in a linear geometry to one Nb5+ and one C1- atom. The C–C bond length is 1.26 Å.
(Cs)2CsYBr6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium-133 molecules and one CsYBr6 framework. In the CsYBr6 framework, Cs1+ is bonded to six equivalent Br1- atoms to form CsBr6 octahedra that share corners with six equivalent YBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Br bond lengths are 3.43 Å. Y3+ is bonded to six equivalent Br1- atoms to form YBr6 octahedra that share corners with six equivalent CsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Y–Br bond lengths are 2.80 Å. Br1- is bonded in a linear geometry to one Cs1+ and one Y3+ atom.
(Cs)2CsSbBr6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight cesium molecules and one CsSbBr6 framework. In the CsSbBr6 framework, Cs1+ is bonded to six equivalent Br1- atoms to form CsBr6 octahedra that share corners with six equivalent SbBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–Br bond lengths are 3.41 Å. Sb3+ is bonded to six equivalent Br1- atoms to form SbBr6 octahedra that share corners with six equivalent CsBr6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–Br bond lengths are 2.82 Å. Br1- is bonded in a linear geometry to one Cs1+ and one Sb3+ atom.