cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1677165
title: Materials Data on Li2VOF4 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1677166
title: Materials Data on Eu2W2O5 by Materials Project

description: Eu2W2O5 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are two inequivalent Eu3+ sites. In the first Eu3+ site, Eu3+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Eu–O bond lengths are 2.67 Å. In the second Eu3+ site, Eu3+ is bonded to twelve O2- atoms to form EuO12 cuboctahedra that share corners with four equivalent EuO12 cuboctahedra, faces with four equivalent EuO12 cuboctahedra, and faces with eight equivalent WO5 square pyramids. There are eight shorter (2.89 Å) and four longer (2.91 Å) Eu–O bond lengths. W2+ is bonded to five O2- atoms to form WO5 square pyramids that share corners with five equivalent WO5 square pyramids and faces with four equivalent EuO12 cuboctahedra. There are four shorter (2.06 Å) and one longer (2.12 Å) W–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four Eu3+ and two equivalent W2+ atoms to form a mixture of distorted edge, face, and corner-sharing OEu4W2 octahedra. The corner-sharing octahedra tilt angles range from 0–66°. In the second O2- site, O2- is bonded to four equivalent Eu3+ and two equivalent W2+ atoms to form a mixture of distorted edge, face, and corner-sharing OEu4W2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.
DOI: 10.17188/1677167
title: Materials Data on YTiFe11 by Materials Project

description: YFe11Ti crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Y is bonded in a 12-coordinate geometry to one Ti and nineteen Fe atoms. The Y–Ti bond length is 3.17 Å. There are a spread of Y–Fe bond distances ranging from 2.96–3.27 Å. Ti is bonded in a 1-coordinate geometry to one Y and thirteen Fe atoms. There are a spread of Ti–Fe bond distances ranging from 2.36–2.89 Å. There are six inequivalent Fe sites. In the first Fe site, Fe is bonded to two equivalent Y, one Ti, and nine Fe atoms to form distorted FeY2TiFe9 cuboctahedra that share corners with twelve FeY2TiFe9 cuboctahedra, edges with five FeY2Fe10 cuboctahedra, and faces with eight FeY2TiFe9 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.35–2.61 Å. In the second Fe site, Fe is bonded to two equivalent Y and ten Fe atoms to form distorted FeY2Fe10 cuboctahedra that share corners with eight equivalent FeY2TiFe9 cuboctahedra, edges with six FeY2Fe10 cuboctahedra, and faces with eight equivalent FeY2TiFe9 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.59–2.72 Å. In the third Fe site, Fe is bonded in a 12-coordinate geometry to two equivalent Y, two equivalent Ti, and eight Fe atoms. There are two shorter (2.64 Å) and two longer (2.69 Å) Fe–Fe bond lengths. In the fourth Fe site, Fe is bonded in a 12-coordinate geometry to two equivalent Y, one Ti, and nine Fe atoms. There are two shorter (2.63 Å) and one longer (2.67 Å) Fe–Fe bond lengths. In the fifth Fe site, Fe is bonded in a 1-coordinate geometry to one Y, one Ti, and twelve Fe atoms. All Fe–Fe bond lengths are 2.93 Å. In the sixth Fe site, Fe is bonded in a 12-coordinate geometry to one Y, two equivalent Ti, and eleven Fe atoms. The Fe–Fe bond length is 2.44 Å.
DOI: 10.17188/1677168
title: Materials Data on Cu(CO2)4 by Materials Project

description: Cu(C2O4)2 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of one Cu(C2O4)2 sheet oriented in the (1, 0, 0) direction. Cu2+ is bonded in an octahedral geometry to six O2- atoms. There are a spread of Cu–O bond distances ranging from 2.07–2.54 Å. There are two inequivalent C+3.50+ sites. In the first C+3.50+ site, C+3.50+ is bonded in a bent 150 degrees geometry to two O2- atoms. Both C–O bond lengths are 1.22 Å. In the second C+3.50+ site, C+3.50+ is bonded in a linear geometry to two O2- atoms. Both C–O bond lengths are 1.18 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cu2+ and one C+3.50+ atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cu2+ and one C+3.50+ atom. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cu2+ and one C+3.50+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C+3.50+ atom.
DOI: 10.17188/1677169
title: Materials Data on Li9Ag4 by Materials Project

description: Li9Ag4 is gamma-brass-like structured and crystallizes in the orthorhombic Fmm2 space group. The structure is three-dimensional. there are seven inequivalent Li sites. In the first Li site, Li is bonded in a 5-coordinate geometry to three Li and five Ag atoms. There are two shorter (2.86 Å) and one longer (2.97 Å) Li–Li bond lengths. There are a spread of Li–Ag bond distances ranging from 2.77–2.82 Å. In the second Li site, Li is bonded in a 4-coordinate geometry to three Li and four Ag atoms. There are one shorter (2.76 Å) and two longer (2.87 Å) Li–Li bond lengths. There are a spread of Li–Ag bond distances ranging from 2.77–2.80 Å. In the third Li site, Li is bonded in a 11-coordinate geometry to seven Li and four Ag atoms. There are a spread of Li–Li bond distances ranging from 2.81–2.95 Å. There are a spread of Li–Ag bond distances ranging from 2.79–3.03 Å. In the fourth Li site, Li is bonded in a 2-coordinate geometry to six Li and five Ag atoms. There are a spread of Li–Li bond distances ranging from 2.77–3.00 Å. There are a spread of Li–Ag bond distances ranging from 2.73–3.11 Å. In the fifth Li site, Li is bonded in a 11-coordinate geometry to five Li and six Ag atoms. Both Li–Li bond lengths are 2.82 Å. There are a spread of Li–Ag bond distances ranging from 2.72–3.15 Å. In the sixth Li site, Li is bonded in a 11-coordinate geometry to six Li and five Ag atoms. The Li–Li bond length is 2.84 Å. There are a spread of Li–Ag bond distances ranging from 2.77–3.10 Å. In the seventh Li site, Li is bonded in a distorted trigonal non-coplanar geometry to six Li and three Ag atoms. There are two shorter (2.83 Å) and one longer (2.85 Å) Li–Ag bond lengths. There are four inequivalent Ag sites. In the first Ag site, Ag is bonded in a 9-coordinate geometry to nine Li and three Ag atoms. There are one shorter (2.96 Å) and two longer (2.97 Å) Ag–Ag bond lengths. In the second Ag site, Ag is bonded in a 11-coordinate geometry to eleven Li and two Ag atoms. The Ag–Ag bond length is 2.87 Å. In the third Ag site, Ag is bonded in a 4-coordinate geometry to ten Li and three Ag atoms. The Ag–Ag bond length is 2.85 Å. In the fourth Ag site, Ag is bonded in a 12-coordinate geometry to twelve Li and one Ag atom.
DOI: 10.17188/1677170
title: Materials Data on Rb(SiPt)4 by Materials Project

description: Rb(PtSi)4 crystallizes in the tetragonal I4 space group. The structure is three-dimensional. Rb1+ is bonded in a 8-coordinate geometry to eight equivalent Pt+0.25- atoms. There are four shorter (3.31 Å) and four longer (3.44 Å) Rb–Pt bond lengths. Pt+0.25- is bonded in a 5-coordinate geometry to two equivalent Rb1+ and five equivalent Si atoms. There are a spread of Pt–Si bond distances ranging from 2.42–2.57 Å. Si is bonded in a 5-coordinate geometry to five equivalent Pt+0.25- atoms.
DOI: 10.17188/1677171
title: Materials Data on SmYFe17 by Materials Project

description: SmYFe17 crystallizes in the trigonal R3m space group. The structure is three-dimensional. Sm is bonded in a 10-coordinate geometry to nineteen Fe atoms. There are a spread of Sm–Fe bond distances ranging from 3.04–3.29 Å. Y is bonded in a 10-coordinate geometry to nineteen Fe atoms. There are a spread of Y–Fe bond distances ranging from 3.03–3.28 Å. There are six inequivalent Fe sites. In the first Fe site, Fe is bonded to one Sm, one Y, and ten Fe atoms to form FeSmYFe10 cuboctahedra that share corners with fourteen FeSmY2Fe9 cuboctahedra, edges with six FeSmY2Fe9 cuboctahedra, and faces with ten FeSmYFe10 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.43–2.61 Å. In the second Fe site, Fe is bonded in a 12-coordinate geometry to one Sm, one Y, and ten Fe atoms. There are a spread of Fe–Fe bond distances ranging from 2.47–2.76 Å. In the third Fe site, Fe is bonded in a 2-coordinate geometry to one Sm and thirteen Fe atoms. There are one shorter (2.41 Å) and three longer (2.65 Å) Fe–Fe bond lengths. In the fourth Fe site, Fe is bonded in a 2-coordinate geometry to one Y and thirteen Fe atoms. All Fe–Fe bond lengths are 2.64 Å. In the fifth Fe site, Fe is bonded to one Sm, two equivalent Y, and nine Fe atoms to form FeSmY2Fe9 cuboctahedra that share corners with fifteen FeSmYFe10 cuboctahedra, edges with eight FeSm2YFe9 cuboctahedra, and faces with ten FeSmYFe10 cuboctahedra. Both Fe–Fe bond lengths are 2.48 Å. In the sixth Fe site, Fe is bonded to two equivalent Sm, one Y, and nine Fe atoms to form FeSm2YFe9 cuboctahedra that share corners with fifteen FeSmYFe10 cuboctahedra, edges with eight FeSm2YFe9 cuboctahedra, and faces with ten FeSmYFe10 cuboctahedra.
DOI: 10.17188/1677172
title: Materials Data on DyB12 by Materials Project

description: DyB12 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a 1-coordinate geometry to twenty-four equivalent B atoms. All Dy–B bond lengths are 2.79 Å. B is bonded in a 7-coordinate geometry to two equivalent Dy and five equivalent B atoms. There is one shorter (1.72 Å) and four longer (1.79 Å) B–B bond length.
DOI: 10.17188/1677173
title: Materials Data on FeBiO3 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1677174
title: Materials Data on BeC2 by Materials Project

description: BeC2 is Copper structured and crystallizes in the cubic Pn-3m space group. The structure is zero-dimensional and consists of four dimethylberyllium molecules. Be2+ is bonded in a linear geometry to two equivalent C1- atoms. Both Be–C bond lengths are 1.63 Å. C1- is bonded in a single-bond geometry to one Be2+ atom.
DOI: 10.17188/1677176
title: Materials Data on LiGeN by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1677177
title: Materials Data on Fe2O3 by Materials Project

description: Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
DOI: 10.17188/1677178
title: Materials Data on ZrS2O13 by Materials Project

description: ZrS2O11O2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two oxygen molecules and one ZrS2O11 cluster. In the ZrS2O11 cluster, Zr is bonded in a 5-coordinate geometry to six O atoms. There are a spread of Zr–O bond distances ranging from 1.88–2.81 Å. There are two inequivalent S sites. In the first S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.45–1.55 Å. In the second S site, S is bonded in a tetrahedral geometry to four O atoms. There are a spread of S–O bond distances ranging from 1.45–1.53 Å. There are eleven inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Zr atom. In the second O site, O is bonded in a bent 150 degrees geometry to one Zr and one S atom. In the third O site, O is bonded in a water-like geometry to one Zr and one S atom. In the fourth O site, O is bonded in a water-like geometry to one Zr and one S atom. In the fifth O site, O is bonded in a single-bond geometry to one O atom. The O–O bond length is 1.23 Å. In the sixth O site, O is bonded in a water-like geometry to one Zr and one O atom. In the seventh O site, O is bonded in a single-bond geometry to one S atom. In the eighth O site, O is bonded in a single-bond geometry to one S atom. In the ninth O site, O is bonded in a single-bond geometry to one S atom. In the tenth O site, O is bonded in a bent 150 degrees geometry to one Zr and one S atom. In the eleventh O site, O is bonded in a single-bond geometry to one S atom.
DOI: 10.17188/1677179
title: Materials Data on La(BOs)2 by Materials Project

description: La(OsB)2 crystallizes in the orthorhombic Fddd space group. The structure is three-dimensional. La3+ is bonded in a 4-coordinate geometry to four equivalent Os+1.50- atoms. All La–Os bond lengths are 3.06 Å. Os+1.50- is bonded in a 4-coordinate geometry to two equivalent La3+ and four equivalent B atoms. There are two shorter (2.11 Å) and two longer (2.18 Å) Os–B bond lengths. B is bonded to four equivalent Os+1.50- atoms to form a mixture of distorted edge and corner-sharing BOs4 trigonal pyramids.
DOI: 10.17188/1677180
title: Materials Data on MnInAgPd by Materials Project

description: MnPdAgIn is Tungsten-derived structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mn is bonded in a body-centered cubic geometry to four equivalent Pd and four equivalent Ag atoms. All Mn–Pd bond lengths are 2.83 Å. All Mn–Ag bond lengths are 2.83 Å. Pd is bonded in a body-centered cubic geometry to four equivalent Mn and four equivalent In atoms. All Pd–In bond lengths are 2.83 Å. Ag is bonded in a distorted body-centered cubic geometry to four equivalent Mn and four equivalent In atoms. All Ag–In bond lengths are 2.83 Å. In is bonded in a distorted body-centered cubic geometry to four equivalent Pd and four equivalent Ag atoms.
DOI: 10.17188/1677181
title: Materials Data on La4Fe(CoO4)3 by Materials Project

description: La4Fe(CoO4)3 is Orthorhombic Perovskite-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are two inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 3-coordinate geometry to nine O2- atoms. There are a spread of La–O bond distances ranging from 2.42–2.80 Å. In the second La3+ site, La3+ is bonded in a 3-coordinate geometry to nine O2- atoms. There are a spread of La–O bond distances ranging from 2.41–2.85 Å. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six CoO6 octahedra. The corner-sharing octahedra tilt angles range from 20–21°. There are a spread of Fe–O bond distances ranging from 1.98–2.03 Å. There are three inequivalent Co3+ sites. In the first Co3+ site, Co3+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with two equivalent CoO6 octahedra and corners with four equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 21–22°. There is four shorter (1.93 Å) and two longer (2.06 Å) Co–O bond length. In the second Co3+ site, Co3+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with two equivalent FeO6 octahedra and corners with four equivalent CoO6 octahedra. The corner-sharing octahedra tilt angles range from 20–21°. There are four shorter (2.02 Å) and two longer (2.05 Å) Co–O bond lengths. In the third Co3+ site, Co3+ is bonded to six O2- atoms to form corner-sharing CoO6 octahedra. The corner-sharing octahedra tilt angles range from 21–22°. There are a spread of Co–O bond distances ranging from 1.92–1.95 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to three La3+, one Fe3+, and one Co3+ atom. In the second O2- site, O2- is bonded in a 5-coordinate geometry to three La3+ and two Co3+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to three La3+, one Fe3+, and one Co3+ atom. In the fourth O2- site, O2- is bonded in a 5-coordinate geometry to three La3+ and two Co3+ atoms. In the fifth O2- site, O2- is bonded in a 5-coordinate geometry to three La3+ and two Co3+ atoms. In the sixth O2- site, O2- is bonded in a 5-coordinate geometry to three La3+, one Fe3+, and one Co3+ atom.
DOI: 10.17188/1677182
title: Materials Data on Sr3ReN3 by Materials Project

description: Sr3ReN3 crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. Sr2+ is bonded to five equivalent N3- atoms to form a mixture of distorted edge and corner-sharing SrN5 trigonal bipyramids. There are a spread of Sr–N bond distances ranging from 2.71–2.91 Å. Re3+ is bonded in a trigonal planar geometry to three equivalent N3- atoms. All Re–N bond lengths are 1.85 Å. N3- is bonded to five equivalent Sr2+ and one Re3+ atom to form a mixture of distorted edge and corner-sharing NSr5Re octahedra. The corner-sharing octahedra tilt angles range from 20–43°.
DOI: 10.17188/1677183
title: Materials Data on Rb2Na2Sb2O3F10 by Materials Project

description: Rb2Na2Sb2O3F10 crystallizes in the monoclinic P2_1/m space group. The structure is three-dimensional. Rb is bonded to twelve F atoms to form distorted RbF12 cuboctahedra that share corners with four equivalent RbF12 cuboctahedra, faces with four equivalent RbF12 cuboctahedra, faces with four equivalent NaOF5 octahedra, and faces with four equivalent SbF5 square pyramids. There are a spread of Rb–F bond distances ranging from 2.89–3.18 Å. Na is bonded to one O and five F atoms to form distorted NaOF5 octahedra that share a cornercorner with one NaOF5 octahedra, corners with five equivalent SbF5 square pyramids, and faces with four equivalent RbF12 cuboctahedra. The corner-sharing octahedral tilt angles are 59°. The Na–O bond length is 2.81 Å. There are a spread of Na–F bond distances ranging from 2.26–2.76 Å. Sb is bonded to five F atoms to form distorted SbF5 square pyramids that share corners with five equivalent NaOF5 octahedra and faces with four equivalent RbF12 cuboctahedra. The corner-sharing octahedra tilt angles range from 6–27°. There are one shorter (2.03 Å) and four longer (2.10 Å) Sb–F bond lengths. There are three inequivalent O sites. In the first O site, O is bonded in a tetrahedral geometry to two equivalent Na and two O atoms. Both O–O bond lengths are 1.31 Å. In the second O site, O is bonded in a single-bond geometry to one O atom. In the third O site, O is bonded in a single-bond geometry to one O atom. There are five inequivalent F sites. In the first F site, F is bonded in a 4-coordinate geometry to two equivalent Rb, one Na, and one Sb atom. In the second F site, F is bonded in a 1-coordinate geometry to four equivalent Rb, one Na, and one Sb atom. In the third F site, F is bonded in a distorted rectangular see-saw-like geometry to two equivalent Rb, one Na, and one Sb atom. In the fourth F site, F is bonded in a distorted rectangular see-saw-like geometry to two equivalent Rb, one Na, and one Sb atom. In the fifth F site, F is bonded in a distorted rectangular see-saw-like geometry to two equivalent Rb, one Na, and one Sb atom.
DOI: 10.17188/1677184
title: Materials Data on Cs2KAuCl6 by Materials Project

description: Cs2KAuCl6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs1+ is bonded to twelve equivalent Cl1- atoms to form CsCl12 cuboctahedra that share corners with twelve equivalent CsCl12 cuboctahedra, faces with six equivalent CsCl12 cuboctahedra, faces with four equivalent KCl6 octahedra, and faces with four equivalent AuCl6 octahedra. All Cs–Cl bond lengths are 3.93 Å. K1+ is bonded to six equivalent Cl1- atoms to form KCl6 octahedra that share corners with six equivalent AuCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All K–Cl bond lengths are 3.02 Å. Au3+ is bonded to six equivalent Cl1- atoms to form AuCl6 octahedra that share corners with six equivalent KCl6 octahedra and faces with eight equivalent CsCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–Cl bond lengths are 2.52 Å. Cl1- is bonded in a distorted linear geometry to four equivalent Cs1+, one K1+, and one Au3+ atom.
DOI: 10.17188/1677186
title: Materials Data on Ca2GaAg by Materials Project

description: Ca2AgGa crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Ca sites. In the first Ca site, Ca is bonded in a 7-coordinate geometry to three equivalent Ag and four equivalent Ga atoms. There are two shorter (3.18 Å) and one longer (3.35 Å) Ca–Ag bond lengths. All Ca–Ga bond lengths are 3.19 Å. In the second Ca site, Ca is bonded in a 7-coordinate geometry to four equivalent Ag and three equivalent Ga atoms. All Ca–Ag bond lengths are 3.20 Å. There are two shorter (3.22 Å) and one longer (3.30 Å) Ca–Ga bond lengths. Ag is bonded in a 9-coordinate geometry to seven Ca and two equivalent Ga atoms. Both Ag–Ga bond lengths are 2.76 Å. Ga is bonded in a 9-coordinate geometry to seven Ca and two equivalent Ag atoms.
DOI: 10.17188/1677187
title: Materials Data on Rb3EuCl6 by Materials Project

description: Rb3EuCl6 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.14–3.87 Å. In the second Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.42–4.05 Å. In the third Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.25–3.88 Å. There are two inequivalent Eu3+ sites. In the first Eu3+ site, Eu3+ is bonded in an octahedral geometry to six Cl1- atoms. There are two shorter (2.69 Å) and four longer (2.74 Å) Eu–Cl bond lengths. In the second Eu3+ site, Eu3+ is bonded in an octahedral geometry to six Cl1- atoms. There are two shorter (2.69 Å) and four longer (2.74 Å) Eu–Cl bond lengths. There are six inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Eu3+ atom. In the second Cl1- site, Cl1- is bonded in a 1-coordinate geometry to five Rb1+ and one Eu3+ atom. In the third Cl1- site, Cl1- is bonded in a 1-coordinate geometry to four Rb1+ and one Eu3+ atom. In the fourth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Eu3+ atom. In the fifth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Eu3+ atom. In the sixth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four Rb1+ and one Eu3+ atom.