cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1680438
title: Materials Data on MnCoSb by Materials Project

description: CoMnSb is half-Heusler structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. Mn2+ is bonded to four equivalent Co1+ and four equivalent Sb3- atoms to form distorted MnCo4Sb4 tetrahedra that share corners with twelve equivalent SbMn4Co6 tetrahedra, edges with twelve equivalent MnCo4Sb4 tetrahedra, and faces with four equivalent SbMn4Co6 tetrahedra. All Mn–Co bond lengths are 2.52 Å. All Mn–Sb bond lengths are 2.52 Å. Co1+ is bonded in a 10-coordinate geometry to four equivalent Mn2+ and six equivalent Sb3- atoms. All Co–Sb bond lengths are 2.91 Å. Sb3- is bonded to four equivalent Mn2+ and six equivalent Co1+ atoms to form distorted SbMn4Co6 tetrahedra that share corners with six equivalent SbMn4Co6 tetrahedra, corners with twelve equivalent MnCo4Sb4 tetrahedra, faces with four equivalent MnCo4Sb4 tetrahedra, and faces with twelve equivalent SbMn4Co6 tetrahedra.
DOI: 10.17188/1680439
title: Materials Data on SrPr(FeO3)2 by Materials Project

description: SrPr(FeO3)2 is Orthorhombic Perovskite-derived structured and crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. Sr2+ is bonded in a 12-coordinate geometry to twelve O2- atoms. There are a spread of Sr–O bond distances ranging from 2.50–3.09 Å. Pr4+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Pr–O bond distances ranging from 2.42–2.57 Å. Fe3+ is bonded to six O2- atoms to form corner-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 16–25°. There are a spread of Fe–O bond distances ranging from 1.98–2.01 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Sr2+, one Pr4+, and two equivalent Fe3+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Sr2+, one Pr4+, and two equivalent Fe3+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Sr2+, one Pr4+, and two equivalent Fe3+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Sr2+, one Pr4+, and two equivalent Fe3+ atoms.
DOI: 10.17188/1680440
title: Materials Data on PrInPd by Materials Project

description: PrPdIn crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Pr is bonded in a 11-coordinate geometry to five Pd and six equivalent In atoms. There are four shorter (3.13 Å) and one longer (3.21 Å) Pr–Pd bond lengths. There are two shorter (3.35 Å) and four longer (3.47 Å) Pr–In bond lengths. There are two inequivalent Pd sites. In the first Pd site, Pd is bonded in a 9-coordinate geometry to three equivalent Pr and six equivalent In atoms. All Pd–In bond lengths are 2.83 Å. In the second Pd site, Pd is bonded in a 9-coordinate geometry to six equivalent Pr and three equivalent In atoms. All Pd–In bond lengths are 2.98 Å. In is bonded in a 10-coordinate geometry to six equivalent Pr and four Pd atoms.
DOI: 10.17188/1680441
title: Materials Data on K3TaNbCu3S8 by Materials Project

description: K3TaNbCu3S8 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are three inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a body-centered cubic geometry to eight S2- atoms. There are a spread of K–S bond distances ranging from 3.32–3.55 Å. In the second K1+ site, K1+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of K–S bond distances ranging from 3.23–3.68 Å. In the third K1+ site, K1+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of K–S bond distances ranging from 3.23–3.67 Å. Ta5+ is bonded to four S2- atoms to form TaS4 tetrahedra that share edges with three CuS4 tetrahedra. There are a spread of Ta–S bond distances ranging from 2.29–2.31 Å. Nb5+ is bonded to four S2- atoms to form NbS4 tetrahedra that share edges with three CuS4 tetrahedra. There are a spread of Nb–S bond distances ranging from 2.29–2.32 Å. There are four inequivalent Cu1+ sites. In the first Cu1+ site, Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with two equivalent CuS4 tetrahedra and edges with two equivalent TaS4 tetrahedra. There are a spread of Cu–S bond distances ranging from 2.33–2.38 Å. In the second Cu1+ site, Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with two equivalent CuS4 tetrahedra and edges with two equivalent NbS4 tetrahedra. There are a spread of Cu–S bond distances ranging from 2.33–2.38 Å. In the third Cu1+ site, Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with four equivalent CuS4 tetrahedra and edges with two equivalent TaS4 tetrahedra. There are two shorter (2.36 Å) and two longer (2.37 Å) Cu–S bond lengths. In the fourth Cu1+ site, Cu1+ is bonded to four S2- atoms to form CuS4 tetrahedra that share corners with four equivalent CuS4 tetrahedra and edges with two equivalent NbS4 tetrahedra. There are two shorter (2.35 Å) and two longer (2.37 Å) Cu–S bond lengths. There are eight inequivalent S2- sites. In the first S2- site, S2- is bonded in a 5-coordinate geometry to three K1+, one Ta5+, and one Cu1+ atom. In the second S2- site, S2- is bonded in a 5-coordinate geometry to three K1+, one Nb5+, and one Cu1+ atom. In the third S2- site, S2- is bonded in a 5-coordinate geometry to two K1+, one Ta5+, and two Cu1+ atoms. In the fourth S2- site, S2- is bonded in a 5-coordinate geometry to two K1+, one Nb5+, and two Cu1+ atoms. In the fifth S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent K1+, one Ta5+, and two Cu1+ atoms. In the sixth S2- site, S2- is bonded in a 5-coordinate geometry to two equivalent K1+, one Nb5+, and two Cu1+ atoms. In the seventh S2- site, S2- is bonded in a 6-coordinate geometry to four K1+, one Ta5+, and one Cu1+ atom. In the eighth S2- site, S2- is bonded to four K1+, one Nb5+, and one Cu1+ atom to form a mixture of distorted corner and edge-sharing SK4NbCu octahedra. The corner-sharing octahedral tilt angles are 69°.
DOI: 10.17188/1680442
title: Materials Data on Be2Tl2Ni(O3F4)2 by Materials Project

description: Be2NiTl2(O3F4)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Be is bonded to four F atoms to form BeF4 tetrahedra that share corners with four equivalent TlOF4 square pyramids. There are a spread of Be–F bond distances ranging from 1.54–1.68 Å. Ni is bonded in a square co-planar geometry to four O atoms. There is two shorter (1.77 Å) and two longer (2.08 Å) Ni–O bond length. Tl is bonded to one O and four F atoms to form distorted TlOF4 square pyramids that share corners with four equivalent BeF4 tetrahedra. The Tl–O bond length is 2.03 Å. There are a spread of Tl–F bond distances ranging from 2.11–2.46 Å. There are three inequivalent O sites. In the first O site, O is bonded in a bent 120 degrees geometry to one Ni and one Tl atom. In the second O site, O is bonded in a bent 120 degrees geometry to one Ni and one O atom. The O–O bond length is 1.24 Å. In the third O site, O is bonded in a single-bond geometry to one O atom. There are four inequivalent F sites. In the first F site, F is bonded in a distorted bent 150 degrees geometry to one Be and one Tl atom. In the second F site, F is bonded in a distorted linear geometry to one Be and one Tl atom. In the third F site, F is bonded in a distorted bent 150 degrees geometry to one Be and one Tl atom. In the fourth F site, F is bonded in a bent 150 degrees geometry to one Be and one Tl atom.
DOI: 10.17188/1680443
title: Materials Data on BaLa2Ti3O10 by Materials Project

description: BaLa2Ti3O10 crystallizes in the orthorhombic Ama2 space group. The structure is three-dimensional. Ba2+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. There are a spread of Ba–O bond distances ranging from 2.72–2.74 Å. There are two inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 12-coordinate geometry to eleven O2- atoms. There are a spread of La–O bond distances ranging from 2.54–2.95 Å. In the second La3+ site, La3+ is bonded to twelve O2- atoms to form distorted LaO12 cuboctahedra that share corners with two equivalent LaO12 cuboctahedra, faces with two equivalent LaO12 cuboctahedra, and faces with four equivalent TiO6 octahedra. There are a spread of La–O bond distances ranging from 2.48–2.93 Å. There are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with four equivalent TiO6 octahedra and faces with four equivalent LaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–11°. There are a spread of Ti–O bond distances ranging from 1.89–2.04 Å. In the second 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 1.78–2.27 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to four La3+ and two Ti4+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to three equivalent Ba2+ and one Ti4+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to two La3+ and two equivalent Ti4+ atoms. In the fourth O2- site, O2- is bonded in a distorted linear geometry to four La3+ and two equivalent Ti4+ atoms. In the fifth O2- site, O2- is bonded in a distorted linear geometry to three La3+ and two equivalent Ti4+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent La3+ and two equivalent Ti4+ atoms. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent La3+ and two equivalent Ti4+ atoms.
DOI: 10.17188/1680445
title: Materials Data on HfNbRe2 by Materials Project

description: HfNbRe2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HfNbRe2 ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to two equivalent Re atoms. Both Hf–Re bond lengths are 2.45 Å. Nb is bonded in a linear geometry to two equivalent Re atoms. Both Nb–Re bond lengths are 2.36 Å. Re is bonded in a linear geometry to one Hf and one Nb atom.
DOI: 10.17188/1680446
title: Materials Data on EuCrTeO6 by Materials Project

description: EuCrTeO6 is beta Vanadium nitride-derived structured and crystallizes in the trigonal P-31c space group. The structure is three-dimensional. Eu2+ is bonded to six equivalent O2- atoms to form EuO6 octahedra that share corners with six equivalent CrO6 octahedra and edges with three equivalent TeO6 octahedra. The corner-sharing octahedral tilt angles are 61°. All Eu–O bond lengths are 2.34 Å. Cr6+ is bonded to six equivalent O2- atoms to form CrO6 octahedra that share corners with six equivalent EuO6 octahedra and corners with six equivalent TeO6 octahedra. The corner-sharing octahedra tilt angles range from 39–61°. All Cr–O bond lengths are 2.09 Å. Te4+ is bonded to six equivalent O2- atoms to form TeO6 octahedra that share corners with six equivalent CrO6 octahedra and edges with three equivalent EuO6 octahedra. The corner-sharing octahedral tilt angles are 39°. All Te–O bond lengths are 1.97 Å. O2- is bonded in a distorted trigonal planar geometry to one Eu2+, one Cr6+, and one Te4+ atom.
DOI: 10.17188/1680447
title: Materials Data on KVSO7 by Materials Project

description: KVSO7 crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional. K is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of K–O bond distances ranging from 2.84–3.15 Å. V is bonded to six O atoms to form distorted VO6 octahedra that share corners with two equivalent VO6 octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 38°. There are a spread of V–O bond distances ranging from 1.64–2.18 Å. S is bonded to four O atoms to form SO4 tetrahedra that share corners with two equivalent VO6 octahedra. The corner-sharing octahedra tilt angles range from 27–49°. There are a spread of S–O bond distances ranging from 1.46–1.54 Å. There are seven inequivalent O sites. In the first O site, O is bonded in a distorted single-bond geometry to one K and one V atom. In the second O site, O is bonded in a distorted single-bond geometry to one K and one S atom. In the third O site, O is bonded in a bent 150 degrees geometry to two equivalent V atoms. In the fourth O site, O is bonded in a distorted bent 150 degrees geometry to one K, one V, and one S atom. In the fifth O site, O is bonded in a distorted single-bond geometry to two equivalent K and one V atom. In the sixth O site, O is bonded in a 2-coordinate geometry to one K, one V, and one S atom. In the seventh O site, O is bonded in a distorted single-bond geometry to three equivalent K and one S atom.
DOI: 10.17188/1680448
title: Materials Data on KMg6Sb by Materials Project

description: KMg6Sb crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. K is bonded to ten Mg and two equivalent Sb atoms to form KMg10Sb2 cuboctahedra that share corners with four equivalent SbK2Mg10 cuboctahedra, corners with six equivalent KMg10Sb2 cuboctahedra, corners with eight equivalent MgK2Mg8Sb2 cuboctahedra, edges with two equivalent SbK2Mg10 cuboctahedra, edges with four equivalent MgK2Mg8Sb2 cuboctahedra, faces with two equivalent KMg10Sb2 cuboctahedra, faces with two equivalent SbK2Mg10 cuboctahedra, and faces with four equivalent MgK2Mg8Sb2 cuboctahedra. There are a spread of K–Mg bond distances ranging from 3.30–3.42 Å. Both K–Sb bond lengths are 3.31 Å. There are four inequivalent Mg sites. In the first Mg site, Mg is bonded to two equivalent K, eight Mg, and two equivalent Sb atoms to form distorted MgK2Mg8Sb2 cuboctahedra that share corners with four equivalent KMg10Sb2 cuboctahedra, corners with four equivalent SbK2Mg10 cuboctahedra, corners with ten equivalent MgK2Mg8Sb2 cuboctahedra, edges with two equivalent KMg10Sb2 cuboctahedra, edges with two equivalent MgK2Mg8Sb2 cuboctahedra, edges with two equivalent SbK2Mg10 cuboctahedra, faces with two equivalent KMg10Sb2 cuboctahedra, faces with two equivalent SbK2Mg10 cuboctahedra, and faces with four equivalent MgK2Mg8Sb2 cuboctahedra. There are a spread of Mg–Mg bond distances ranging from 3.24–3.34 Å. There are one shorter (3.38 Å) and one longer (3.44 Å) Mg–Sb bond lengths. In the second Mg site, Mg is bonded in a 12-coordinate geometry to two equivalent K, two equivalent Mg, and two equivalent Sb atoms. Both Mg–Sb bond lengths are 3.25 Å. In the third Mg site, Mg is bonded in a 2-coordinate geometry to two equivalent K and four equivalent Mg atoms. In the fourth Mg site, Mg is bonded in a distorted water-like geometry to four equivalent Mg and two equivalent Sb atoms. Both Mg–Sb bond lengths are 3.33 Å. Sb is bonded to two equivalent K and ten Mg atoms to form SbK2Mg10 cuboctahedra that share corners with four equivalent KMg10Sb2 cuboctahedra, corners with six equivalent SbK2Mg10 cuboctahedra, corners with eight equivalent MgK2Mg8Sb2 cuboctahedra, edges with two equivalent KMg10Sb2 cuboctahedra, edges with four equivalent MgK2Mg8Sb2 cuboctahedra, faces with two equivalent KMg10Sb2 cuboctahedra, faces with two equivalent SbK2Mg10 cuboctahedra, and faces with four equivalent MgK2Mg8Sb2 cuboctahedra.
DOI: 10.17188/1680449
title: Materials Data on LiVF4 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: 10.17188/1680450
title: Materials Data on Co11CuO16 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: 10.17188/1680451
title: Materials Data on NaSbN2 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: 10.17188/1680452
title: Materials Data on Mg2InN2 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: 10.17188/1680453
title: Materials Data on Li2CoGeO4 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: 10.17188/1680454
title: Materials Data on FeO2 by Materials Project

description: FeO2 crystallizes in the orthorhombic Cmcm space group. The structure is two-dimensional and consists of two FeO2 sheets oriented in the (0, 1, 0) direction. Fe is bonded to six O atoms to form a mixture of edge and corner-sharing FeO6 octahedra. The corner-sharing octahedral tilt angles are 30°. There are a spread of Fe–O bond distances ranging from 1.95–2.09 Å. There are two inequivalent O sites. In the first O site, O is bonded to four equivalent Fe atoms to form a mixture of edge and corner-sharing OFe4 trigonal pyramids. In the second O site, O is bonded in a water-like geometry to two equivalent Fe atoms.
DOI: 10.25403/upresearchdata.13297862
title: The influence of agile project teams and team voice on product innovation in a large South African Investment bank

description: This research data consists of recordings, transcripts and data coding. Some files will need a .DS store file opener to view them while some interview recordings are stored as M4A files.
DOI: 10.25403/upresearchdata.13297862.v1
title: The influence of agile project teams and team voice on product innovation in a large South African Investment bank

description: This research data consists of recordings, transcripts and data coding. Some files will need a .DS store file opener to view them while some interview recordings are stored as M4A files.
DOI: 10.17188/1680456
title: Materials Data on Mg3Cu2(SiO4)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: 10.17188/1680457
title: Materials Data on Li7V3P8O29 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: 10.17188/1680458
title: Materials Data on Rb2LiScCl6 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: 10.17188/1680459
title: Materials Data on KIO3 by Materials Project

description: KIO3 crystallizes in the trigonal R3 space group. The structure is three-dimensional. K1+ is bonded in a 9-coordinate geometry to nine equivalent O2- atoms. There are a spread of K–O bond distances ranging from 2.99–3.26 Å. O2- is bonded in a distorted single-bond geometry to three equivalent K1+ and two equivalent I5+ atoms. There are one shorter (1.84 Å) and one longer (2.72 Å) O–I bond lengths. I5+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms.
DOI: 10.17188/1680460
title: Materials Data on Li2AlCoO4 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: 10.17188/1680461
title: Materials Data on Cr2Ni by Materials Project

description: Cr2Ni is Cubic Laves structured and crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Cr is bonded to six equivalent Cr and six equivalent Ni atoms to form a mixture of edge, corner, and face-sharing CrCr6Ni6 cuboctahedra. All Cr–Cr bond lengths are 2.32 Å. All Cr–Ni bond lengths are 2.72 Å. Ni is bonded in a 12-coordinate geometry to twelve equivalent Cr and four equivalent Ni atoms. All Ni–Ni bond lengths are 2.84 Å.
DOI: 10.17188/1680462
title: Materials Data on Zr7VO16 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: 10.17188/1680463
title: Materials Data on CrCu3(PO4)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: 10.17188/1680464
title: Materials Data on Al(SO6)2 by Materials Project

description: Al(SO5)2O2 crystallizes in the orthorhombic Pnma space group. The structure is two-dimensional and consists of four oxygen molecules and two Al(SO5)2 sheets oriented in the (0, 0, 1) direction. In each Al(SO5)2 sheet, Al is bonded to six O atoms to form AlO6 octahedra that share corners with four equivalent SO4 tetrahedra. There are a spread of Al–O bond distances ranging from 1.88–1.92 Å. S is bonded to four O atoms to form SO4 tetrahedra that share corners with two equivalent AlO6 octahedra. The corner-sharing octahedra tilt angles range from 42–46°. There are a spread of S–O bond distances ranging from 1.46–1.51 Å. There are five inequivalent O sites. In the first O site, O is bonded in a distorted bent 120 degrees geometry to one Al and one S atom. In the second O site, O is bonded in a single-bond geometry to one S atom. In the third O site, O is bonded in a single-bond geometry to one Al atom. In the fourth O site, O is bonded in a bent 150 degrees geometry to one Al and one S atom. In the fifth O site, O is bonded in a single-bond geometry to one S atom.
DOI: 10.17188/1680465
title: Materials Data on Eu5P3O12F by Materials Project

description: Eu5(PO4)3F crystallizes in the hexagonal P6_3/m space group. The structure is three-dimensional. there are two inequivalent Eu2+ sites. In the first Eu2+ site, Eu2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Eu–O bond distances ranging from 2.58–2.95 Å. In the second Eu2+ site, Eu2+ is bonded in a 7-coordinate geometry to six O2- and one F1- atom. There are a spread of Eu–O bond distances ranging from 2.52–2.80 Å. The Eu–F bond length is 2.43 Å. P5+ is bonded in a tetrahedral geometry to four O2- atoms. There is three shorter (1.56 Å) and one longer (1.57 Å) P–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three Eu2+ and one P5+ atom. In the second O2- site, O2- is bonded in a 1-coordinate geometry to three Eu2+ and one P5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to three Eu2+ and one P5+ atom. F1- is bonded in a trigonal planar geometry to three equivalent Eu2+ atoms.