cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1655083
title: Materials Data on Zr6Al16Pt7 by Materials Project

description: Zr6Pt7Al16 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Zr is bonded in a 4-coordinate geometry to four equivalent Zr, four equivalent Pt, and eight Al atoms. All Zr–Zr bond lengths are 3.27 Å. All Zr–Pt bond lengths are 3.21 Å. There are four shorter (2.92 Å) and four longer (3.21 Å) Zr–Al bond lengths. There are two inequivalent Pt sites. In the first Pt site, Pt is bonded to four equivalent Zr and eight Al atoms to form distorted PtZr4Al8 cuboctahedra that share corners with four equivalent PtZr4Al8 cuboctahedra, corners with eight equivalent AlZr3Pt4 tetrahedra, edges with four equivalent AlZr3Pt4 tetrahedra, and faces with eight equivalent PtZr4Al8 cuboctahedra. There are four shorter (2.54 Å) and four longer (2.73 Å) Pt–Al bond lengths. In the second Pt site, Pt is bonded in a body-centered cubic geometry to eight equivalent Al atoms. All Pt–Al bond lengths are 2.59 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded in a 3-coordinate geometry to three equivalent Zr and three equivalent Pt atoms. In the second Al site, Al is bonded to three equivalent Zr and four Pt atoms to form distorted AlZr3Pt4 tetrahedra that share corners with six equivalent PtZr4Al8 cuboctahedra, corners with seven equivalent AlZr3Pt4 tetrahedra, edges with three equivalent PtZr4Al8 cuboctahedra, edges with three equivalent AlZr3Pt4 tetrahedra, and faces with three equivalent AlZr3Pt4 tetrahedra.
DOI: 10.17188/1655084
title: Materials Data on LiNO2 by Materials Project

description: LiNO2 crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Li1+ is bonded to six equivalent O2- atoms to form a mixture of distorted edge and corner-sharing LiO6 pentagonal pyramids. There are four shorter (2.26 Å) and two longer (2.33 Å) Li–O bond lengths. N3+ is bonded in a bent 120 degrees geometry to two equivalent O2- atoms. Both N–O bond lengths are 1.27 Å. O2- is bonded to three equivalent Li1+ and one N3+ atom to form a mixture of distorted edge and corner-sharing OLi3N tetrahedra.
DOI: 10.17188/1655086
title: Materials Data on AsS by Materials Project

description: SAs crystallizes in the orthorhombic Cmc2_1 space group. The structure is one-dimensional and consists of two SAs ribbons oriented in the (0, 0, 1) direction. there are two inequivalent As2+ sites. In the first As2+ site, As2+ is bonded in a 6-coordinate geometry to six S2- atoms. There are a spread of As–S bond distances ranging from 2.44–2.93 Å. In the second As2+ site, As2+ is bonded in an L-shaped geometry to two S2- atoms. There are one shorter (2.29 Å) and one longer (2.36 Å) As–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to four As2+ atoms to form distorted corner-sharing SAs4 trigonal pyramids. In the second S2- site, S2- is bonded in a 2-coordinate geometry to three As2+ atoms.
DOI: 10.17188/1655087
title: Materials Data on NaNiAsO4 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: 10.17188/1655088
title: Materials Data on Fe2OF3 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: 10.17188/1655089
title: Materials Data on Pb7O16 by Materials Project

description: Pb7O16 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are five inequivalent Pb sites. In the first Pb site, Pb is bonded to six O atoms to form a mixture of edge and corner-sharing PbO6 octahedra. The corner-sharing octahedra tilt angles range from 53–57°. There are a spread of Pb–O bond distances ranging from 2.18–2.26 Å. In the second Pb site, Pb is bonded to six O atoms to form a mixture of edge and corner-sharing PbO6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There are a spread of Pb–O bond distances ranging from 2.14–2.28 Å. In the third Pb site, Pb is bonded to six O atoms to form a mixture of edge and corner-sharing PbO6 octahedra. The corner-sharing octahedra tilt angles range from 52–56°. There are a spread of Pb–O bond distances ranging from 2.18–2.24 Å. In the fourth Pb site, Pb is bonded to six O atoms to form a mixture of edge and corner-sharing PbO6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There are a spread of Pb–O bond distances ranging from 2.15–2.28 Å. In the fifth Pb site, Pb is bonded to six O atoms to form a mixture of edge and corner-sharing PbO6 octahedra. The corner-sharing octahedra tilt angles range from 51–57°. There are a spread of Pb–O bond distances ranging from 2.18–2.27 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to three Pb atoms. In the second O site, O is bonded in a trigonal planar geometry to three Pb atoms. In the third O site, O is bonded in a bent 120 degrees geometry to two Pb atoms. In the fourth O site, O is bonded in a trigonal planar geometry to three Pb atoms. In the fifth O site, O is bonded in a water-like geometry to two Pb atoms. In the sixth O site, O is bonded in a trigonal planar geometry to three Pb atoms. In the seventh O site, O is bonded in a trigonal planar geometry to three Pb atoms. In the eighth O site, O is bonded in a bent 120 degrees geometry to two Pb atoms.
DOI: 10.17188/1655090
title: Materials Data on SrCdAu by Materials Project

description: SrAuCd crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Sr is bonded in a 5-coordinate geometry to five equivalent Au atoms. There are two shorter (3.28 Å) and three longer (3.33 Å) Sr–Au bond lengths. Au is bonded in a 9-coordinate geometry to five equivalent Sr and four equivalent Cd atoms. There are a spread of Au–Cd bond distances ranging from 2.93–3.07 Å. Cd is bonded in a 4-coordinate geometry to four equivalent Au atoms.
DOI: 10.17188/1655091
title: Materials Data on Cu3Ru by Materials Project

description: RuCu3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ru is bonded to twelve Cu atoms to form RuCu12 cuboctahedra that share corners with six equivalent RuCu12 cuboctahedra, corners with twelve CuCu8Ru4 cuboctahedra, edges with eighteen CuCu8Ru4 cuboctahedra, faces with eight equivalent RuCu12 cuboctahedra, and faces with twelve CuCu8Ru4 cuboctahedra. There are six shorter (2.61 Å) and six longer (2.63 Å) Ru–Cu bond lengths. There are two inequivalent Cu sites. In the first Cu site, Cu is bonded to four equivalent Ru and eight Cu atoms to form distorted CuCu8Ru4 cuboctahedra that share corners with four equivalent RuCu12 cuboctahedra, corners with fourteen CuCu8Ru4 cuboctahedra, edges with six equivalent RuCu12 cuboctahedra, edges with twelve CuCu8Ru4 cuboctahedra, faces with four equivalent RuCu12 cuboctahedra, and faces with sixteen CuCu8Ru4 cuboctahedra. There are a spread of Cu–Cu bond distances ranging from 2.58–2.67 Å. In the second Cu site, Cu is bonded to four equivalent Ru and eight Cu atoms to form distorted CuCu8Ru4 cuboctahedra that share corners with four equivalent RuCu12 cuboctahedra, corners with fourteen CuCu8Ru4 cuboctahedra, edges with six equivalent RuCu12 cuboctahedra, edges with twelve CuCu8Ru4 cuboctahedra, faces with four equivalent RuCu12 cuboctahedra, and faces with sixteen CuCu8Ru4 cuboctahedra. Both Cu–Cu bond lengths are 2.58 Å.
DOI: 10.17188/1655092
title: Materials Data on Li4Co5SnO12 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: 10.17188/1655093
title: Materials Data on Mn2P12W by Materials Project

description: WMn2P12 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. W6+ is bonded in a 8-coordinate geometry to eight P+0.83- atoms. There are a spread of W–P bond distances ranging from 2.49–2.64 Å. Mn2+ is bonded to six P+0.83- atoms to form MnP6 octahedra that share corners with four equivalent PP3W tetrahedra and an edgeedge with one MnP6 octahedra. There are a spread of Mn–P bond distances ranging from 2.20–2.30 Å. There are six inequivalent P+0.83- sites. In the first P+0.83- site, P+0.83- is bonded in a 1-coordinate geometry to one W6+, one Mn2+, and two P+0.83- atoms. There are one shorter (2.21 Å) and one longer (2.23 Å) P–P bond lengths. In the second P+0.83- site, P+0.83- is bonded in a 1-coordinate geometry to one W6+, one Mn2+, and two P+0.83- atoms. There are one shorter (2.29 Å) and one longer (2.31 Å) P–P bond lengths. In the third P+0.83- site, P+0.83- is bonded in a distorted single-bond geometry to one W6+, one Mn2+, and two P+0.83- atoms. There are one shorter (2.24 Å) and one longer (2.31 Å) P–P bond lengths. In the fourth P+0.83- site, P+0.83- is bonded in a 2-coordinate geometry to two equivalent Mn2+ and two P+0.83- atoms. The P–P bond length is 2.21 Å. In the fifth P+0.83- site, P+0.83- is bonded to one W6+ and three P+0.83- atoms to form distorted PP3W tetrahedra that share corners with four equivalent MnP6 octahedra and a cornercorner with one PP3W tetrahedra. The corner-sharing octahedra tilt angles range from 54–74°. In the sixth P+0.83- site, P+0.83- is bonded in a distorted single-bond geometry to one Mn2+ and three P+0.83- atoms. The P–P bond length is 2.20 Å.
DOI: 10.17188/1655094
title: Materials Data on Ga2(WO4)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: 10.17188/1655095
title: Materials Data on Rb2MnH12(SeO7)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: 10.17188/1655097
title: Materials Data on Mg10FeO11 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: 10.17188/1655098
title: Materials Data on FeBi3(MoO6)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: 10.17188/1655099
title: Materials Data on SrOs7N10 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: 10.17188/1655100
title: Materials Data on TbU3(CoGe)8 by Materials Project

description: U3Tb(CoGe)8 crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are two inequivalent U sites. In the first U site, U is bonded in a 8-coordinate geometry to eight Co and eight Ge atoms. All U–Co bond lengths are 3.16 Å. There are four shorter (3.10 Å) and four longer (3.11 Å) U–Ge bond lengths. In the second U site, U is bonded in a 8-coordinate geometry to eight equivalent Co and eight equivalent Ge atoms. All U–Co bond lengths are 3.18 Å. All U–Ge bond lengths are 3.11 Å. Tb is bonded in a 8-coordinate geometry to eight equivalent Co and eight equivalent Ge atoms. All Tb–Co bond lengths are 3.21 Å. All Tb–Ge bond lengths are 3.11 Å. There are two inequivalent Co sites. In the first Co site, Co is bonded to two equivalent U, two equivalent Tb, and four Ge atoms to form a mixture of distorted edge, face, and corner-sharing CoTb2U2Ge4 tetrahedra. There are two shorter (2.32 Å) and two longer (2.35 Å) Co–Ge bond lengths. In the second Co site, Co is bonded to four U and four Ge atoms to form distorted CoU4Ge4 tetrahedra that share corners with twelve CoTb2U2Ge4 tetrahedra, edges with six CoTb2U2Ge4 tetrahedra, and faces with four equivalent CoU4Ge4 tetrahedra. All Co–Ge bond lengths are 2.34 Å. There are four inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to four equivalent Tb, four equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.55 Å. In the second Ge site, Ge is bonded in a 9-coordinate geometry to four equivalent U, four equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.51 Å. In the third Ge site, Ge is bonded in a 9-coordinate geometry to four equivalent U, four equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.51 Å. In the fourth Ge site, Ge is bonded in a 9-coordinate geometry to four equivalent U, four equivalent Co, and one Ge atom.
DOI: 10.17188/1655101
title: Materials Data on P3CN2Cl13 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: 10.17188/1655103
title: Materials Data on LaMn3V4O12 by Materials Project

description: LaV4Mn3O12 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. La3+ is bonded to twelve O2- atoms to form LaO12 cuboctahedra that share faces with eight VO6 octahedra. There are a spread of La–O bond distances ranging from 2.60–2.71 Å. There are four inequivalent V+3.75+ sites. In the first V+3.75+ site, V+3.75+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six VO6 octahedra and faces with two equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 34–41°. There are a spread of V–O bond distances ranging from 1.98–2.09 Å. In the second V+3.75+ site, V+3.75+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six VO6 octahedra and faces with two equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 34–39°. There are a spread of V–O bond distances ranging from 1.98–2.07 Å. In the third V+3.75+ site, V+3.75+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six VO6 octahedra and faces with two equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 34–39°. There are a spread of V–O bond distances ranging from 1.93–2.02 Å. In the fourth V+3.75+ site, V+3.75+ is bonded to six O2- atoms to form VO6 octahedra that share corners with six VO6 octahedra and faces with two equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 34–41°. There are a spread of V–O bond distances ranging from 1.91–2.01 Å. There are three inequivalent Mn2+ sites. In the first Mn2+ site, Mn2+ is bonded in a square co-planar geometry to four O2- atoms. There is two shorter (1.97 Å) and two longer (1.98 Å) Mn–O bond length. In the second Mn2+ site, Mn2+ is bonded in a distorted square co-planar geometry to four O2- atoms. There are two shorter (2.11 Å) and two longer (2.12 Å) Mn–O bond lengths. In the third Mn2+ site, Mn2+ is bonded in a distorted square co-planar geometry to four O2- atoms. There are two shorter (2.12 Å) and two longer (2.13 Å) Mn–O bond lengths. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one La3+, two V+3.75+, and one Mn2+ atom.
DOI: 10.17188/1655105
title: Materials Data on AlCuS2 by Materials Project

description: CuAlS2 is Ilmenite-like structured and crystallizes in the trigonal R3m space group. The structure is three-dimensional. Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with nine equivalent AlS6 octahedra, corners with six equivalent CuS4 tetrahedra, and a faceface with one AlS6 octahedra. The corner-sharing octahedra tilt angles range from 51–61°. There are one shorter (2.26 Å) and three longer (2.36 Å) Cu–S bond lengths. Al3+ is bonded to six S2- atoms to form AlS6 octahedra that share corners with nine equivalent CuS4 tetrahedra, edges with six equivalent AlS6 octahedra, and a faceface with one CuS4 tetrahedra. There are three shorter (2.39 Å) and three longer (2.56 Å) Al–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to one Cu1+ and three equivalent Al3+ atoms to form distorted corner-sharing SAl3Cu tetrahedra. In the second S2- site, S2- is bonded in a 6-coordinate geometry to three equivalent Cu1+ and three equivalent Al3+ atoms.
DOI: 10.17188/1655106
title: Materials Data on Li2MnPCO7 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: 10.17188/1655107
title: Materials Data on LiFe2OF3 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: 10.17188/1655108
title: Materials Data on TmC8N4Cl7 by Materials Project

description: TmC4N2Cl5(ClCCN)2 crystallizes in the orthorhombic P2_12_12 space group. The structure is one-dimensional and consists of four chloromethyl(methylidyne)azanium molecules and two TmC4N2Cl5 ribbons oriented in the (0, 1, 0) direction. In each TmC4N2Cl5 ribbon, Tm3+ is bonded in a distorted tetrahedral geometry to four Cl1- atoms. There are two shorter (2.43 Å) and two longer (2.56 Å) Tm–Cl bond lengths. There are two inequivalent C2+ sites. In the first C2+ site, C2+ is bonded in a water-like geometry to one N3- and one Cl1- atom. The C–N bond length is 1.25 Å. The C–Cl bond length is 2.33 Å. In the second C2+ site, C2+ is bonded in a bent 120 degrees geometry to one N3- and one Cl1- atom. The C–N bond length is 1.27 Å. The C–Cl bond length is 1.96 Å. N3- is bonded in a linear geometry to two C2+ atoms. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Tm3+ atom. In the second Cl1- site, Cl1- is bonded in a bent 150 degrees geometry to two equivalent C2+ atoms. In the third Cl1- site, Cl1- is bonded in a water-like geometry to one Tm3+ and one C2+ atom.
DOI: 10.17188/1655109
title: Materials Data on TbTa3O9 by Materials Project

description: TbTa3O9 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. Tb3+ is bonded to twelve O2- atoms to form TbO12 cuboctahedra that share corners with three equivalent TbO12 cuboctahedra, faces with two equivalent TbO12 cuboctahedra, and faces with eight TaO6 octahedra. There are a spread of Tb–O bond distances ranging from 2.52–2.89 Å. There are three inequivalent Ta5+ sites. In the first Ta5+ site, Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with six TaO6 octahedra and faces with three equivalent TbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–18°. There are a spread of Ta–O bond distances ranging from 1.93–2.05 Å. In the second Ta5+ site, Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with six TaO6 octahedra and faces with two equivalent TbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–15°. There is two shorter (1.97 Å) and four longer (1.99 Å) Ta–O bond length. In the third Ta5+ site, Ta5+ is bonded to six O2- atoms to form TaO6 octahedra that share corners with six TaO6 octahedra and faces with three equivalent TbO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 3–18°. There are a spread of Ta–O bond distances ranging from 1.91–2.08 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a linear geometry to two equivalent Tb3+ and two equivalent Ta5+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Tb3+ and two Ta5+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Tb3+ and two Ta5+ atoms. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to three equivalent Tb3+ and two Ta5+ atoms. In the fifth O2- site, O2- is bonded in a linear geometry to two equivalent Ta5+ atoms. In the sixth O2- site, O2- is bonded in a linear geometry to two Ta5+ atoms. In the seventh O2- site, O2- is bonded in a 2-coordinate geometry to one Tb3+ and two Ta5+ atoms.
DOI: 10.17188/1655110
title: Materials Data on LiZn4(SnO2)4 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: 10.17188/1655112
title: Materials Data on Cr4Si2Br2O7 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: 10.17188/1655113
title: Materials Data on Dy2(Al3Rh)3 by Materials Project

description: Dy2(RhAl3)3 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Dy is bonded in a 11-coordinate geometry to eleven Al atoms. There are a spread of Dy–Al bond distances ranging from 3.05–3.13 Å. There are two inequivalent Rh sites. In the first Rh site, Rh is bonded in a 8-coordinate geometry to eight Al atoms. There are a spread of Rh–Al bond distances ranging from 2.56–2.63 Å. In the second Rh site, Rh is bonded in a 8-coordinate geometry to eight Al atoms. There are a spread of Rh–Al bond distances ranging from 2.55–2.61 Å. There are four inequivalent Al sites. In the first Al site, Al is bonded in a 2-coordinate geometry to two equivalent Dy and two equivalent Rh atoms. In the second Al site, Al is bonded in a 3-coordinate geometry to three equivalent Dy and three Rh atoms. In the third Al site, Al is bonded in a 3-coordinate geometry to two equivalent Dy and three Rh atoms. In the fourth Al site, Al is bonded in a 2-coordinate geometry to two equivalent Dy and two equivalent Rh atoms.