cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1744820
title: Materials Data on Hg(MoS2)6 by Materials Project

description: Hg(MoS2)6 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of one mercury molecule and four MoS2 clusters. In two of the MoS2 clusters, Mo+3.67+ is bonded in a 1-coordinate geometry to two S2- atoms. Both Mo–S bond lengths are 2.32 Å. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded in a distorted single-bond geometry to one Mo+3.67+ and one S2- atom. The S–S bond length is 2.08 Å. In the second S2- site, S2- is bonded in a 1-coordinate geometry to one Mo+3.67+ and one S2- atom. In two of the MoS2 clusters, there are two inequivalent Mo+3.67+ sites. In the first Mo+3.67+ site, Mo+3.67+ is bonded in a 1-coordinate geometry to two S2- atoms. Both Mo–S bond lengths are 2.32 Å. In the second Mo+3.67+ site, Mo+3.67+ is bonded in a 1-coordinate geometry to two S2- atoms. There are one shorter (2.31 Å) and one longer (2.32 Å) Mo–S bond lengths. There are four inequivalent S2- sites. In the first S2- site, S2- is bonded in a 2-coordinate geometry to one Mo+3.67+ and one S2- atom. The S–S bond length is 2.08 Å. In the second S2- site, S2- is bonded in a 1-coordinate geometry to one Mo+3.67+ and one S2- atom. The S–S bond length is 2.08 Å. In the third S2- site, S2- is bonded in a distorted single-bond geometry to one Mo+3.67+ and two S2- atoms. The S–S bond length is 4.07 Å. In the fourth S2- site, S2- is bonded in a distorted single-bond geometry to one Mo+3.67+ and two S2- atoms.
DOI: 10.17188/1744821
title: Materials Data on Y3MnB7 by Materials Project

description: Y3MnB7 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. there are two inequivalent Y sites. In the first Y site, Y is bonded in a 11-coordinate geometry to eleven B atoms. There are a spread of Y–B bond distances ranging from 2.61–2.73 Å. In the second Y site, Y is bonded in a 12-coordinate geometry to ten B atoms. There are a spread of Y–B bond distances ranging from 2.61–2.68 Å. Mn is bonded in a 10-coordinate geometry to ten B atoms. There are a spread of Mn–B bond distances ranging from 2.27–2.29 Å. There are four inequivalent B sites. In the first B site, B is bonded in a 9-coordinate geometry to six Y and three B atoms. There is one shorter (1.90 Å) and two longer (1.96 Å) B–B bond length. In the second B site, B is bonded in a 9-coordinate geometry to four Y, two equivalent Mn, and three B atoms. There is one shorter (1.78 Å) and one longer (1.81 Å) B–B bond length. In the third B site, B is bonded in a 9-coordinate geometry to four equivalent Y, two equivalent Mn, and three B atoms. There is one shorter (1.72 Å) and one longer (1.96 Å) B–B bond length. In the fourth B site, B is bonded in a 8-coordinate geometry to four equivalent Y, two equivalent Mn, and two equivalent B atoms.
DOI: 10.17188/1744822
title: Materials Data on MgMn8(OF)8 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: 10.17188/1744823
title: Materials Data on Rb2Ti(TeO4)3 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: 10.25390/caryinstitute.11560068.v1
title: Cary Environmental Monitoring Program Hourly Meteorological and Solar Radiation Data: 1988-2019

description: The Cary Institute of Ecosystem Studies Environmental Monitoring Program is a long-term data collection program designed to understand how the environment changes over time. The program includes monitoring of climate including temperature and precipitation, as well as variables related to air pollution, such as acid deposition and ozone, and water pollution and other streamwater chemistry. Our solar radiation monitoring includes diffuse and global photosynthetically active radiation (PAR), diffuse and global shortwave radiation, net radiation and UV. Long-term monitoring of solar radiation provides us with an understanding of atmospheric energy dynamics, which can affect natural and human systems. The Cary Institute of Ecosystem Studies, Environmental Monitoring Program furnishes data under the following conditions: The data have received quality assurance scrutiny by our program, and, although we are confident of the accuracy of these data, the Cary Institute will not be held liable for errors in these data. Data are subject to change resulting from updates in data screening or models used. Data citation: The following is a standard citation for referencing data from the Cary Institute of Ecosystem Studies, Environmental Monitoring Program:Cary Institute of Ecosystem Studies, Environmental Monitoring Program. 2008 (or current year). Cary Institute of Ecosystem Studies, Box AB, Millbrook, NY 12545, www.caryinstitute.org.Those wishing to publish data from the Cary Institute of Ecosystem Studies, Environmental Monitoring Program are encouraged to contact Data Manager Vicky Kelly, kellyv@caryinstitute.org.
DOI: 10.17188/1744824
title: Materials Data on Pr6Ge3Se14 by Materials Project

description: Pr6Ge3Se14 crystallizes in the trigonal P3 space group. The structure is three-dimensional. there are two inequivalent Pr3+ sites. In the first Pr3+ site, Pr3+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Pr–Se bond distances ranging from 3.00–3.35 Å. In the second Pr3+ site, Pr3+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Pr–Se bond distances ranging from 3.00–3.30 Å. There are three inequivalent Ge+3.33+ sites. In the first Ge+3.33+ site, Ge+3.33+ is bonded in a tetrahedral geometry to four Se2- atoms. There are one shorter (2.35 Å) and three longer (2.41 Å) Ge–Se bond lengths. In the second Ge+3.33+ site, Ge+3.33+ is bonded in a tetrahedral geometry to four Se2- atoms. There are one shorter (2.35 Å) and three longer (2.40 Å) Ge–Se bond lengths. In the third Ge+3.33+ site, Ge+3.33+ is bonded in an octahedral geometry to six Se2- atoms. There are three shorter (2.82 Å) and three longer (2.86 Å) Ge–Se bond lengths. There are six inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a tetrahedral geometry to three equivalent Pr3+ and one Ge+3.33+ atom. In the second Se2- site, Se2- is bonded in a tetrahedral geometry to three equivalent Pr3+ and one Ge+3.33+ atom. In the third Se2- site, Se2- is bonded in a distorted rectangular see-saw-like geometry to three Pr3+ and one Ge+3.33+ atom. In the fourth Se2- site, Se2- is bonded in a distorted rectangular see-saw-like geometry to three Pr3+ and one Ge+3.33+ atom. In the fifth Se2- site, Se2- is bonded in a 5-coordinate geometry to four Pr3+ and one Ge+3.33+ atom. In the sixth Se2- site, Se2- is bonded in a 5-coordinate geometry to four Pr3+ and one Ge+3.33+ atom.
DOI: 10.17188/1744825
title: Materials Data on BaB2O9 by Materials Project

description: BaB2O9 crystallizes in the monoclinic P2_1/c space group. The structure is two-dimensional and consists of one BaB2O9 sheet oriented in the (1, 0, 0) direction. Ba is bonded in a 8-coordinate geometry to eight O atoms. There are a spread of Ba–O bond distances ranging from 2.65–3.14 Å. There are two inequivalent B sites. In the first B site, B is bonded in a trigonal planar geometry to three O atoms. There is one shorter (1.35 Å) and two longer (1.39 Å) B–O bond length. In the second B site, B is bonded in a tetrahedral geometry to four O atoms. There are a spread of B–O bond distances ranging from 1.42–1.47 Å. There are nine inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to one Ba and one B atom. In the second O site, O is bonded in a single-bond geometry to one B atom. In the third O site, O is bonded in a single-bond geometry to one Ba and one B atom. In the fourth O site, O is bonded in a single-bond geometry to one Ba and one B 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 distorted single-bond geometry to two equivalent Ba and one B atom. In the seventh O site, O is bonded in a single-bond geometry to one Ba and one B atom. In the eighth O site, O is bonded in a bent 120 degrees geometry to one Ba and one O atom. In the ninth O site, O is bonded in a single-bond geometry to one Ba and one B atom.
DOI: 10.17188/1744826
title: Materials Data on VZn(SiO3)2 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: 10.17188/1744827
title: Materials Data on LiPbN 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: 10.17188/1744828
title: Materials Data on LuNbO4 by Materials Project

description: LuNbO4 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. Lu3+ is bonded to six O2- atoms to form a mixture of distorted corner and edge-sharing LuO6 octahedra. The corner-sharing octahedral tilt angles are 43°. There are a spread of Lu–O bond distances ranging from 2.14–2.36 Å. Nb5+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Nb–O bond distances ranging from 1.83–2.36 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Lu3+ and two equivalent Nb5+ atoms. In the second O2- site, O2- is bonded in a linear geometry to one Lu3+ and one Nb5+ atom. In the third O2- site, O2- is bonded to three equivalent Lu3+ and one Nb5+ atom to form a mixture of corner and edge-sharing OLu3Nb tetrahedra. In the fourth O2- site, O2- is bonded in a distorted T-shaped geometry to one Lu3+ and two equivalent Nb5+ atoms.
DOI: 10.17188/1744829
title: Materials Data on La2Ti3CuO10 by Materials Project

description: La2Ti3CuO10 crystallizes in the tetragonal I-4m2 space group. The structure is three-dimensional. La3+ is bonded to twelve O2- atoms to form distorted LaO12 cuboctahedra that share corners with eight equivalent LaO12 cuboctahedra, faces with five equivalent LaO12 cuboctahedra, and faces with four equivalent TiO6 octahedra. There are a spread of La–O bond distances ranging from 2.51–2.92 Å. There are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Ti–O bond distances ranging from 1.81–2.32 Å. In the second Ti4+ site, Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with four equivalent TiO6 octahedra and faces with eight equivalent LaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. There is four shorter (1.92 Å) and two longer (1.95 Å) Ti–O bond length. Cu2+ is bonded in a 4-coordinate geometry to four equivalent O2- atoms. All Cu–O bond lengths are 2.01 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Ti4+ and two equivalent Cu2+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent La3+ and two equivalent Ti4+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent La3+ and two equivalent Ti4+ atoms. In the fourth O2- site, O2- is bonded in a 1-coordinate geometry to four equivalent La3+ and two Ti4+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to four equivalent La3+ and two equivalent Ti4+ atoms.
DOI: 10.17188/1744830
title: Materials Data on Li2CrFe(PO4)2 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: 10.17188/1744832
title: Materials Data on KAuO3 by Materials Project

description: KAuO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. K1+ is bonded to twelve equivalent O2- atoms to form KO12 cuboctahedra that share corners with twelve equivalent KO12 cuboctahedra, faces with six equivalent KO12 cuboctahedra, and faces with eight equivalent AuO6 octahedra. All K–O bond lengths are 2.94 Å. Au5+ is bonded to six equivalent O2- atoms to form AuO6 octahedra that share corners with six equivalent AuO6 octahedra and faces with eight equivalent KO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–O bond lengths are 2.08 Å. O2- is bonded to four equivalent K1+ and two equivalent Au5+ atoms to form a mixture of distorted face, edge, and corner-sharing OK4Au2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.
DOI: 10.17188/1744833
title: Materials Data on La3Zr by Materials Project

description: La3Zr is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. La is bonded to eight equivalent La and four equivalent Zr atoms to form distorted LaLa8Zr4 cuboctahedra that share corners with four equivalent ZrLa12 cuboctahedra, corners with fourteen equivalent LaLa8Zr4 cuboctahedra, edges with six equivalent ZrLa12 cuboctahedra, edges with twelve equivalent LaLa8Zr4 cuboctahedra, faces with four equivalent ZrLa12 cuboctahedra, and faces with sixteen equivalent LaLa8Zr4 cuboctahedra. There are a spread of La–La bond distances ranging from 3.48–3.73 Å. There are two shorter (3.56 Å) and two longer (3.60 Å) La–Zr bond lengths. Zr is bonded to twelve equivalent La atoms to form ZrLa12 cuboctahedra that share corners with six equivalent ZrLa12 cuboctahedra, corners with twelve equivalent LaLa8Zr4 cuboctahedra, edges with eighteen equivalent LaLa8Zr4 cuboctahedra, faces with eight equivalent ZrLa12 cuboctahedra, and faces with twelve equivalent LaLa8Zr4 cuboctahedra.
DOI: 10.6084/m9.figshare.13567988
title: Data for: Body condition loss during the dry period: Insights from feeding behavior studies

description: Here you will find the original dataset and full data analyses for the manuscript entitled "Body condition loss during the dry period: Insights from feeding behavior studies" by Daros, Havekes and DeVries. This manuscript has been accepted to be published in the Journal of Dairy Science in 2021.
DOI: 10.17188/1744834
title: Materials Data on Li2MnCrO4 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: 10.6084/m9.figshare.13567988.v1
title: Data for: Body condition loss during the dry period: Insights from feeding behavior studies

description: Here you will find the original dataset and full data analyses for the manuscript entitled "Body condition loss during the dry period: Insights from feeding behavior studies" by Daros, Havekes and DeVries. This manuscript has been accepted to be published in the Journal of Dairy Science in 2021.
DOI: 10.17188/1744835
title: Materials Data on InCN2 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: 10.5281/zenodo.3592016
title: 4prim-O-beta-D-apiosyl_glucomatronaline

description: NMR Data of 4'-O-beta-D-apiosyl glucomatronaline 1 1D 1H<br> 3 2D 1H-1H COSY<br> 4 2D 1H-13C HSQC<br> 5 2D 1H-13C HMBC<br> 6 2D 1H-1H ROESY<br> 102 1D 13C{1H}
DOI: 10.17188/1744836
title: Materials Data on YbZnGe by Materials Project

description: YbZnGe crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Yb is bonded in a 12-coordinate geometry to six equivalent Zn and six equivalent Ge atoms. There are a spread of Yb–Zn bond distances ranging from 3.08–3.24 Å. There are a spread of Yb–Ge bond distances ranging from 3.05–3.25 Å. Zn is bonded in a 10-coordinate geometry to six equivalent Yb, one Zn, and three equivalent Ge atoms. The Zn–Zn bond length is 2.57 Å. There are two shorter (2.59 Å) and one longer (2.91 Å) Zn–Ge bond lengths. Ge is bonded in a 10-coordinate geometry to six equivalent Yb, three equivalent Zn, and one Ge atom. The Ge–Ge bond length is 2.59 Å.
DOI: 10.5281/zenodo.3443667
title: 4prim-O-beta-D-apiosyl_glucomatronaline

description: NMR Data of 4'-O-beta-D-apiosyl glucomatronaline 1 1D 1H<br> 3 2D 1H-1H COSY<br> 4 2D 1H-13C HSQC<br> 5 2D 1H-13C HMBC<br> 6 2D 1H-1H ROESY<br> 102 1D 13C{1H}
DOI: 10.17188/1744837
title: Materials Data on Zn2In2O5 by Materials Project

description: Zn2In2O5 is Aluminum carbonitride-like structured and crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are two inequivalent Zn2+ sites. In the first Zn2+ site, Zn2+ is bonded in a 4-coordinate geometry to five O2- atoms. There are a spread of Zn–O bond distances ranging from 2.00–2.61 Å. In the second Zn2+ site, Zn2+ is bonded to four O2- atoms to form ZnO4 tetrahedra that share corners with three equivalent InO6 octahedra, corners with six equivalent ZnO4 tetrahedra, and corners with three equivalent InO5 trigonal bipyramids. The corner-sharing octahedral tilt angles are 62°. There are one shorter (1.98 Å) and three longer (2.10 Å) Zn–O bond lengths. There are two inequivalent In3+ sites. In the first In3+ site, In3+ is bonded to six O2- atoms to form InO6 octahedra that share corners with three equivalent ZnO4 tetrahedra and edges with six equivalent InO6 octahedra. There are three shorter (2.25 Å) and three longer (2.27 Å) In–O bond lengths. In the second In3+ site, In3+ is bonded to five O2- atoms to form InO5 trigonal bipyramids that share corners with three equivalent ZnO4 tetrahedra and corners with six equivalent InO5 trigonal bipyramids. There are a spread of In–O bond distances ranging from 2.01–2.23 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to three equivalent Zn2+ and one In3+ atom to form OZn3In tetrahedra that share corners with ten OZn3In tetrahedra and edges with three equivalent OZnIn3 trigonal pyramids. In the second O2- site, O2- is bonded to one Zn2+ and three equivalent In3+ atoms to form OZnIn3 tetrahedra that share corners with twelve OZn3In tetrahedra, a cornercorner with one OZnIn3 trigonal pyramid, and edges with three equivalent OZnIn3 tetrahedra. In the third O2- site, O2- is bonded to one Zn2+ and three equivalent In3+ atoms to form a mixture of distorted corner and edge-sharing OZnIn3 tetrahedra. In the fourth O2- site, O2- is bonded to three equivalent Zn2+ and one In3+ atom to form OZn3In tetrahedra that share corners with ten OZn3In tetrahedra and corners with three equivalent OZnIn3 trigonal pyramids. In the fifth O2- site, O2- is bonded to one Zn2+ and three equivalent In3+ atoms to form distorted OZnIn3 trigonal pyramids that share corners with four OZnIn3 tetrahedra, corners with six equivalent OZnIn3 trigonal pyramids, and edges with three equivalent OZn3In tetrahedra.
DOI: 10.17188/1744838
title: Materials Data on MgTl2(PO4)4 by Materials Project

description: MgTl2(PO4)4 crystallizes in the triclinic P-1 space group. The structure is two-dimensional and consists of one MgTl2(PO4)4 sheet oriented in the (1, 0, 1) direction. Mg is bonded to six O atoms to form MgO6 octahedra that share corners with four PO4 tetrahedra. There are four shorter (2.05 Å) and two longer (2.17 Å) Mg–O bond lengths. Tl is bonded in a 3-coordinate geometry to three O atoms. There are a spread of Tl–O bond distances ranging from 2.58–2.70 Å. There are two inequivalent P sites. In the first P site, P is bonded to four O atoms to form PO4 tetrahedra that share a cornercorner with one MgO6 octahedra and a cornercorner with one PO4 tetrahedra. The corner-sharing octahedral tilt angles are 44°. There are a spread of P–O bond distances ranging from 1.52–1.62 Å. In the second P site, P is bonded to four O atoms to form PO4 tetrahedra that share a cornercorner with one MgO6 octahedra and a cornercorner with one PO4 tetrahedra. The corner-sharing octahedral tilt angles are 43°. There are a spread of P–O bond distances ranging from 1.52–1.61 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to one Tl and one P atom. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Tl and one P atom. In the third O site, O is bonded in a distorted bent 150 degrees geometry to one Mg and one P atom. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to two P atoms. In the fifth O site, O is bonded in a single-bond geometry to one P atom. In the sixth O site, O is bonded in a distorted bent 150 degrees geometry to one Tl and one P atom. In the seventh O site, O is bonded in a distorted bent 150 degrees geometry to one Mg and one P atom. In the eighth O site, O is bonded in a single-bond geometry to one Mg atom.
DOI: 10.17188/1744839
title: Materials Data on Mn4TeO8 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: 10.17188/1744840
title: Materials Data on ErGePd by Materials Project

description: ErPdGe crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. there are four inequivalent Er sites. In the first Er site, Er is bonded in a 12-coordinate geometry to six Pd and six Ge atoms. All Er–Pd bond lengths are 3.11 Å. There are four shorter (3.07 Å) and two longer (3.21 Å) Er–Ge bond lengths. In the second Er site, Er is bonded in a 12-coordinate geometry to six Pd and six Ge atoms. There are a spread of Er–Pd bond distances ranging from 2.95–3.19 Å. There are a spread of Er–Ge bond distances ranging from 3.02–3.28 Å. In the third Er site, Er is bonded in a 12-coordinate geometry to six Pd and six Ge atoms. There are two shorter (3.19 Å) and four longer (3.24 Å) Er–Pd bond lengths. There are two shorter (2.98 Å) and four longer (3.01 Å) Er–Ge bond lengths. In the fourth Er site, Er is bonded in a 12-coordinate geometry to six Pd and six Ge atoms. There are a spread of Er–Pd bond distances ranging from 3.04–3.14 Å. There are a spread of Er–Ge bond distances ranging from 3.07–3.21 Å. There are three inequivalent Pd sites. In the first Pd site, Pd is bonded in a 10-coordinate geometry to six Er and four Ge atoms. There are a spread of Pd–Ge bond distances ranging from 2.57–2.74 Å. In the second Pd site, Pd is bonded in a 10-coordinate geometry to six Er and four Ge atoms. There are a spread of Pd–Ge bond distances ranging from 2.55–2.92 Å. In the third Pd site, Pd is bonded in a 10-coordinate geometry to six Er, one Pd, and three Ge atoms. The Pd–Pd bond length is 2.99 Å. There are two shorter (2.54 Å) and one longer (2.57 Å) Pd–Ge bond lengths. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 10-coordinate geometry to six Er, three Pd, and one Ge atom. The Ge–Ge bond length is 2.74 Å. In the second Ge site, Ge is bonded in a 10-coordinate geometry to six Er and four Pd atoms. In the third Ge site, Ge is bonded in a 10-coordinate geometry to six Er and four Pd atoms.