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NH4HF2 is High Pressure (4-7GPa) Tellurium structured and crystallizes in the orthorhombic Pmna space group. The structure is zero-dimensional and consists of four ammonium molecules and four hydrogen fluoride hydrogen fluoride molecules.
ReO3 is High-temperature superconductor-like structured and crystallizes in the tetragonal P4/mbm space group. The structure is three-dimensional. Re6+ is bonded to six O2- atoms to form corner-sharing ReO6 octahedra. The corner-sharing octahedra tilt angles range from 0–6°. All Re–O bond lengths are 1.90 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Re6+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent Re6+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two equivalent Re6+ atoms. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent Re6+ atoms.
CdCO3 is High-temperature superconductor-derived structured and crystallizes in the monoclinic C2/m space group. The structure is three-dimensional and consists of two methane molecules and one CdO3 framework. In the CdO3 framework, Cd2+ is bonded to six O2- atoms to form corner-sharing CdO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.07 Å) and four longer (2.08 Å) Cd–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Cd2+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent Cd2+ atoms.
SiO2 is High (Orthorhombic) Tridymite-like structured and crystallizes in the hexagonal P6_522 space group. The structure is three-dimensional. Si4+ is bonded to four O2- atoms to form corner-sharing SiO4 tetrahedra. All Si–O bond lengths are 1.62 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Si4+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent Si4+ atoms.
ClF3 is High Pressure (4-7GPa) Tellurium structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four ClF3 clusters. Cl is bonded in a T-shaped geometry to three F atoms. There is one shorter (1.64 Å) and two longer (1.75 Å) Cl–F bond length. There are two inequivalent F sites. In the first F site, F is bonded in a single-bond geometry to one Cl atom. In the second F site, F is bonded in a single-bond geometry to one Cl atom.
AlPO4 is High (Orthorhombic) Tridymite-derived structured and crystallizes in the hexagonal P6_3cm space group. The structure is three-dimensional. there are two inequivalent Al3+ sites. In the first Al3+ site, Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four PO4 tetrahedra. There are a spread of Al–O bond distances ranging from 1.74–1.76 Å. In the second Al3+ site, Al3+ is bonded to four O2- atoms to form AlO4 tetrahedra that share corners with four PO4 tetrahedra. There is two shorter (1.74 Å) and two longer (1.76 Å) Al–O bond length. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four AlO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.53–1.55 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four AlO4 tetrahedra. There is two shorter (1.53 Å) and two longer (1.54 Å) P–O bond length. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Al3+ and one P5+ atom. In the second O2- site, O2- is bonded in a linear geometry to one Al3+ and one P5+ atom. In the third O2- site, O2- is bonded in a linear geometry to one Al3+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to one Al3+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a bent 120 degrees geometry to one Al3+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a linear geometry to one Al3+ and one P5+ atom. In the seventh O2- site, O2- is bonded in a linear geometry to one Al3+ and one P5+ atom.
WO3 is High-temperature superconductor-like structured and crystallizes in the orthorhombic Pbcm space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form corner-sharing WO6 octahedra. The corner-sharing octahedra tilt angles range from 0–4°. There are a spread of W–O bond distances ranging from 1.85–2.03 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two equivalent W6+ atoms.
W3Si is High-temperature superconductor structured and crystallizes in the cubic Im-3m space group. The structure is three-dimensional. W is bonded to four equivalent W and two equivalent Si atoms to form distorted WSi2W4 octahedra that share corners with six equivalent WSi2W4 octahedra, edges with four equivalent SiW6 octahedra, and edges with eight equivalent WSi2W4 octahedra. The corner-sharing octahedral tilt angles are 0°. All W–W bond lengths are 2.61 Å. Both W–Si bond lengths are 2.61 Å. Si is bonded to six equivalent W atoms to form SiW6 octahedra that share corners with six equivalent SiW6 octahedra and edges with twelve equivalent WSi2W4 octahedra. The corner-sharing octahedral tilt angles are 0°.
TeI4 is High Pressure Cadmuum Telluride-derived structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four TeI4 clusters. there are three inequivalent Te4+ sites. In the first Te4+ site, Te4+ is bonded to six I1- atoms to form edge-sharing TeI6 octahedra. There are a spread of Te–I bond distances ranging from 2.80–3.28 Å. In the second Te4+ site, Te4+ is bonded to six I1- atoms to form edge-sharing TeI6 octahedra. There are a spread of Te–I bond distances ranging from 2.80–3.26 Å. In the third Te4+ site, Te4+ is bonded to six I1- atoms to form edge-sharing TeI6 octahedra. There are a spread of Te–I bond distances ranging from 2.80–3.26 Å. There are ten inequivalent I1- sites. In the first I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the second I1- site, I1- is bonded in a 3-coordinate geometry to three Te4+ atoms. In the third I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the fourth I1- site, I1- is bonded in a water-like geometry to two Te4+ atoms. In the fifth I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the sixth I1- site, I1- is bonded in a water-like geometry to two Te4+ atoms. In the seventh I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the eighth I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the ninth I1- site, I1- is bonded in a single-bond geometry to one Te4+ atom. In the tenth I1- site, I1- is bonded in a 3-coordinate geometry to three Te4+ atoms.
V3Si is High-temperature superconductor structured and crystallizes in the cubic Im-3m space group. The structure is three-dimensional. V is bonded to four equivalent V and two equivalent Si atoms to form VV4Si2 octahedra that share corners with six equivalent VV4Si2 octahedra, edges with four equivalent SiV6 octahedra, and edges with eight equivalent VV4Si2 octahedra. The corner-sharing octahedral tilt angles are 0°. All V–V bond lengths are 2.46 Å. Both V–Si bond lengths are 2.46 Å. Si is bonded to six equivalent V atoms to form SiV6 octahedra that share corners with six equivalent SiV6 octahedra and edges with twelve equivalent VV4Si2 octahedra. The corner-sharing octahedral tilt angles are 0°.
P3N4SOCl5 is High Pressure (4-7GPa) Tellurium structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four P3N4SOCl5 clusters. there are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to two N+1.50- and two Cl1- atoms to form corner-sharing PN2Cl2 tetrahedra. There is one shorter (1.59 Å) and one longer (1.60 Å) P–N bond length. There are one shorter (2.01 Å) and one longer (2.02 Å) P–Cl bond lengths. In the second P5+ site, P5+ is bonded to three N+1.50- and one Cl1- atom to form corner-sharing PN3Cl tetrahedra. There is two shorter (1.60 Å) and one longer (1.68 Å) P–N bond length. The P–Cl bond length is 2.01 Å. There are three inequivalent N+1.50- sites. In the first N+1.50- site, N+1.50- is bonded in a bent 120 degrees geometry to two equivalent P5+ atoms. In the second N+1.50- site, N+1.50- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the third N+1.50- site, N+1.50- is bonded in a bent 120 degrees geometry to one P5+ and one S2- atom. The N–S bond length is 1.53 Å. S2- is bonded in a bent 120 degrees geometry to one N+1.50- and one O2- atom. The S–O bond length is 1.46 Å. O2- is bonded in a single-bond geometry to one S2- atom. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one P5+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one P5+ atom. In the third Cl1- site, Cl1- is bonded in a single-bond geometry to one P5+ atom.
NbO2F is High-temperature superconductor-derived structured and crystallizes in the orthorhombic Imma space group. The structure is three-dimensional. there are two inequivalent Nb5+ sites. In the first Nb5+ site, Nb5+ is bonded to four O2- and two F1- atoms to form corner-sharing NbO4F2 octahedra. The corner-sharing octahedra tilt angles range from 0–9°. There is three shorter (1.94 Å) and one longer (2.01 Å) Nb–O bond length. There are one shorter (1.99 Å) and one longer (2.10 Å) Nb–F bond lengths. In the second Nb5+ site, Nb5+ is bonded to four O2- and two equivalent F1- atoms to form distorted corner-sharing NbO4F2 octahedra. The corner-sharing octahedra tilt angles range from 0–9°. There is two shorter (1.86 Å) and two longer (1.97 Å) Nb–O bond length. Both Nb–F bond lengths are 2.28 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Nb5+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two equivalent Nb5+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two Nb5+ atoms. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent Nb5+ atoms. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two equivalent Nb5+ atoms. In the second F1- site, F1- is bonded in a distorted linear geometry to two Nb5+ atoms.
FeH2O3Cl5 is High Pressure (4-7GPa) Tellurium structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four FeH2O3Cl5 clusters. Fe is bonded in a 6-coordinate geometry to one O and five Cl atoms. The Fe–O bond length is 1.92 Å. There are a spread of Fe–Cl bond distances ranging from 2.29–2.58 Å. H is bonded in a single-bond geometry to one O atom. The H–O bond length is 1.00 Å. There are two inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Fe atom. In the second O site, O is bonded in a single-bond geometry to one H and one Cl atom. The O–Cl bond length is 2.30 Å. There are four inequivalent Cl sites. In the first Cl site, Cl is bonded in a single-bond geometry to one Fe atom. In the second Cl site, Cl is bonded in a distorted trigonal non-coplanar geometry to one Fe and two equivalent O atoms. In the third Cl site, Cl is bonded in a single-bond geometry to one Fe atom. In the fourth Cl site, Cl is bonded in a single-bond geometry to one Fe atom.
LiC8H20O4Cl is High Pressure Cadmuum Telluride-derived structured and crystallizes in the monoclinic C2/c space group. The structure is zero-dimensional and consists of four LiC8H20O4Cl clusters. Li1+ is bonded to four O2- and one Cl1- atom to form LiClO4 trigonal bipyramids that share corners with four CH3O tetrahedra. There are two shorter (2.12 Å) and two longer (2.14 Å) Li–O bond lengths. The Li–Cl bond length is 2.42 Å. There are four inequivalent C+1.50- sites. In the first C+1.50- site, C+1.50- is bonded to three H1+ and one O2- atom to form CH3O tetrahedra that share a cornercorner with one LiClO4 trigonal bipyramid. All C–H bond lengths are 1.10 Å. The C–O bond length is 1.43 Å. In the second C+1.50- site, C+1.50- is bonded in a distorted trigonal non-coplanar geometry to two H1+ and one O2- atom. There is one shorter (1.10 Å) and one longer (1.11 Å) C–H bond length. The C–O bond length is 1.44 Å. In the third C+1.50- site, C+1.50- is bonded in a distorted trigonal non-coplanar geometry to two H1+ and one O2- atom. Both C–H bond lengths are 1.11 Å. The C–O bond length is 1.44 Å. In the fourth C+1.50- site, C+1.50- is bonded to three H1+ and one O2- atom to form CH3O tetrahedra that share a cornercorner with one LiClO4 trigonal bipyramid. All C–H bond lengths are 1.10 Å. The C–O bond length is 1.44 Å. There are ten inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the ninth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. In the tenth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.50- atom. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two C+1.50- atoms. In the second O2- site, O2- is bonded in a trigonal non-coplanar geometry to one Li1+ and two C+1.50- atoms. Cl1- is bonded in a single-bond geometry to one Li1+ atom.
CrN4H14OCl3 is High Pressure (4-7GPa) Tellurium structured and crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four CrN4H14OCl3 clusters. Cr3+ is bonded in an octahedral geometry to four N3-, one O2-, and one Cl1- atom. There are one shorter (2.09 Å) and three longer (2.10 Å) Cr–N bond lengths. The Cr–O bond length is 2.08 Å. The Cr–Cl bond length is 2.35 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Cr3+ and three H1+ atoms. There is one shorter (1.02 Å) and two longer (1.03 Å) N–H bond length. In the second N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Cr3+ and three H1+ atoms. There is one shorter (1.02 Å) and two longer (1.03 Å) N–H bond length. In the third N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Cr3+ and three H1+ atoms. There is one shorter (1.02 Å) and two longer (1.03 Å) N–H bond length. There are eight inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one O2- and one Cl1- atom. The H–O bond length is 1.00 Å. The H–Cl bond length is 2.10 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. O2- is bonded in a distorted trigonal non-coplanar geometry to one Cr3+ and two equivalent H1+ atoms. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Cr3+ atom. In the second Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one H1+ atom.
NbO2F is High-temperature superconductor-derived structured and crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Nb5+ sites. In the first Nb5+ site, Nb5+ is bonded to three O2- and three F1- atoms to form corner-sharing NbO3F3 octahedra. The corner-sharing octahedra tilt angles range from 0–13°. There is one shorter (1.84 Å) and two longer (1.93 Å) Nb–O bond length. There are two shorter (2.02 Å) and one longer (2.20 Å) Nb–F bond lengths. In the second Nb5+ site, Nb5+ is bonded to five O2- and one F1- atom to form corner-sharing NbO5F octahedra. The corner-sharing octahedra tilt angles range from 0–6°. There are a spread of Nb–O bond distances ranging from 1.99–2.02 Å. The Nb–F bond length is 2.10 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Nb5+ atoms. In the second O2- site, O2- is bonded in a linear geometry to two Nb5+ atoms. In the third O2- site, O2- is bonded in a linear geometry to two Nb5+ atoms. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to two equivalent Nb5+ atoms. In the second F1- site, F1- is bonded in a linear geometry to two Nb5+ atoms.
WO2F is High-temperature superconductor-derived structured and crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. W5+ is bonded to four equivalent O2- and two equivalent F1- atoms to form corner-sharing WO4F2 octahedra. The corner-sharing octahedra tilt angles range from 4–6°. There is two shorter (1.87 Å) and two longer (2.02 Å) W–O bond length. Both W–F bond lengths are 2.08 Å. O2- is bonded in a linear geometry to two equivalent W5+ atoms. F1- is bonded in a linear geometry to two equivalent W5+ atoms.
CH3NH3SnI3 is High-temperature superconductor-derived structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional and consists of four methylammonium molecules and one SnI3 framework. In the SnI3 framework, there are four inequivalent Sn4+ sites. In the first Sn4+ site, Sn4+ is bonded to six I1- atoms to form corner-sharing SnI6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are a spread of Sn–I bond distances ranging from 3.06–3.32 Å. In the second Sn4+ site, Sn4+ is bonded to six I1- atoms to form corner-sharing SnI6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are a spread of Sn–I bond distances ranging from 3.05–3.23 Å. In the third Sn4+ site, Sn4+ is bonded to six I1- atoms to form corner-sharing SnI6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are a spread of Sn–I bond distances ranging from 3.06–3.32 Å. In the fourth Sn4+ site, Sn4+ is bonded to six I1- atoms to form corner-sharing SnI6 octahedra. The corner-sharing octahedra tilt angles range from 0–3°. There are a spread of Sn–I bond distances ranging from 3.06–3.26 Å. There are twelve inequivalent I1- sites. In the first I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the second I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the third I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the fourth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the fifth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the sixth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the seventh I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the eighth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the ninth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the tenth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the eleventh I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms. In the twelfth I1- site, I1- is bonded in a linear geometry to two Sn4+ atoms.