cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1662947
title: Materials Data on Na3(CoO2)4 by Materials Project

description: Na3(CoO2)4 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are two inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded to six O2- atoms to form distorted NaO6 pentagonal pyramids that share corners with six CoO6 octahedra, edges with six CoO6 octahedra, and edges with six equivalent NaO6 pentagonal pyramids. The corner-sharing octahedra tilt angles range from 9–13°. There are a spread of Na–O bond distances ranging from 2.38–2.40 Å. In the second Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.42–2.48 Å. There are two inequivalent Co+3.25+ sites. In the first Co+3.25+ site, Co+3.25+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with three equivalent NaO6 pentagonal pyramids, edges with six CoO6 octahedra, and edges with three equivalent NaO6 pentagonal pyramids. There are a spread of Co–O bond distances ranging from 1.95–2.10 Å. In the second Co+3.25+ site, Co+3.25+ is bonded to six O2- atoms to form CoO6 octahedra that share corners with three equivalent NaO6 pentagonal pyramids, edges with six CoO6 octahedra, and edges with three equivalent NaO6 pentagonal pyramids. There are a spread of Co–O bond distances ranging from 1.96–2.09 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to three equivalent Na1+ and three Co+3.25+ atoms to form ONa3Co3 octahedra that share corners with six ONa3Co3 octahedra, corners with three equivalent ONa2Co3 square pyramids, edges with six ONa3Co3 octahedra, an edgeedge with one ONa2Co3 square pyramid, and a faceface with one ONa3Co3 octahedra. The corner-sharing octahedra tilt angles range from 40–43°. In the second O2- site, O2- is bonded to three equivalent Na1+ and three Co+3.25+ atoms to form ONa3Co3 octahedra that share corners with six ONa3Co3 octahedra, edges with six ONa3Co3 octahedra, edges with two equivalent ONa2Co3 square pyramids, and a faceface with one ONa3Co3 octahedra. The corner-sharing octahedra tilt angles range from 40–44°. In the third O2- site, O2- is bonded in a distorted see-saw-like geometry to one Na1+ and three Co+3.25+ atoms. In the fourth O2- site, O2- is bonded to two equivalent Na1+ and three Co+3.25+ atoms to form ONa2Co3 square pyramids that share corners with three equivalent ONa3Co3 octahedra, corners with two equivalent ONa2Co3 square pyramids, edges with three ONa3Co3 octahedra, and edges with three equivalent ONa2Co3 square pyramids. The corner-sharing octahedra tilt angles range from 1–4°.
DOI: 10.17188/1662948
title: Materials Data on Zr2P3(NO7)2 by Materials Project

description: Zr2(PO4)3(NO)2 crystallizes in the monoclinic C2/c space group. The structure is two-dimensional and consists of eight nitroxyl molecules and two Zr2(PO4)3 sheets oriented in the (1, 0, 0) direction. In each Zr2(PO4)3 sheet, Zr+3.50+ is bonded to five O2- atoms to form distorted ZrO5 trigonal bipyramids that share corners with five PO4 tetrahedra. There are a spread of Zr–O bond distances ranging from 1.95–2.09 Å. There are two inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with four equivalent ZrO5 trigonal bipyramids. There is two shorter (1.54 Å) and two longer (1.55 Å) P–O bond length. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent ZrO5 trigonal bipyramids. There are a spread of P–O bond distances ranging from 1.49–1.61 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Zr+3.50+ and one P5+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Zr+3.50+ and one P5+ atom. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to one Zr+3.50+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Zr+3.50+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one P5+ atom. In the sixth O2- site, O2- is bonded in a linear geometry to one Zr+3.50+ and one P5+ atom.
DOI: 10.17188/1662949
title: Materials Data on Sb4Au(Xe2F11)2 by Materials Project

description: Xe4Au(Sb2F11)2 crystallizes in the tetragonal P4_32_12 space group. The structure is zero-dimensional and consists of eight Sb2F11 clusters and four Xe4Au clusters. In each Sb2F11 cluster, there are two inequivalent Sb sites. In the first Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 30°. There are a spread of Sb–F bond distances ranging from 1.89–2.07 Å. In the second Sb site, Sb is bonded to six F atoms to form corner-sharing SbF6 octahedra. The corner-sharing octahedral tilt angles are 30°. There are a spread of Sb–F bond distances ranging from 1.89–2.11 Å. There are eleven inequivalent F sites. In the first F site, F is bonded in a bent 150 degrees geometry to two Sb atoms. In the second F site, F is bonded in a single-bond geometry to one Sb atom. In the third F site, F is bonded in a single-bond geometry to one Sb atom. In the fourth F site, F is bonded in a single-bond geometry to one Sb atom. In the fifth F site, F is bonded in a single-bond geometry to one Sb atom. In the sixth F site, F is bonded in a single-bond geometry to one Sb atom. In the seventh F site, F is bonded in a single-bond geometry to one Sb atom. In the eighth F site, F is bonded in a single-bond geometry to one Sb atom. In the ninth F site, F is bonded in a single-bond geometry to one Sb atom. In the tenth F site, F is bonded in a single-bond geometry to one Sb atom. In the eleventh F site, F is bonded in a single-bond geometry to one Sb atom. In each Xe4Au cluster, there are three inequivalent Xe sites. In the first Xe site, Xe is bonded in a single-bond geometry to one Au atom. The Xe–Au bond length is 2.82 Å. In the second Xe site, Xe is bonded in a single-bond geometry to one Au atom. The Xe–Au bond length is 2.84 Å. In the third Xe site, Xe is bonded in a single-bond geometry to one Au atom. The Xe–Au bond length is 2.77 Å. Au is bonded in a square co-planar geometry to four Xe atoms.
DOI: 10.17188/1662950
title: Materials Data on LiFe3(OF3)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: 10.17188/1662951
title: Materials Data on Cd3(InN2)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: 10.17188/1662952
title: Materials Data on Li5NiO4 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: 10.17188/1662953
title: Materials Data on K3YN6 by Materials Project

description: K3YN6 crystallizes in the trigonal R32 space group. The structure is three-dimensional. there are two inequivalent K1+ sites. In the first K1+ site, K1+ is bonded in a 8-coordinate geometry to eight N1- atoms. There are a spread of K–N bond distances ranging from 2.92–3.34 Å. In the second K1+ site, K1+ is bonded in a 8-coordinate geometry to eight N1- atoms. There are a spread of K–N bond distances ranging from 2.87–3.34 Å. Y3+ is bonded in an octahedral geometry to six N1- atoms. There are three shorter (2.27 Å) and three longer (2.31 Å) Y–N bond lengths. There are two inequivalent N1- sites. In the first N1- site, N1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom. In the second N1- site, N1- is bonded in a 5-coordinate geometry to four K1+ and one Y3+ atom.
DOI: 10.17188/1662954
title: Materials Data on Ni5O4 by Materials Project

description: Ni5O4 crystallizes in the cubic P-43m space group. The structure is three-dimensional. there are two inequivalent Ni+1.60+ sites. In the first Ni+1.60+ site, Ni+1.60+ is bonded to six equivalent O2- atoms to form distorted NiO6 octahedra that share corners with six equivalent NiO6 octahedra, corners with three equivalent NiO4 tetrahedra, edges with twelve equivalent NiO6 octahedra, and a faceface with one NiO4 tetrahedra. The corner-sharing octahedral tilt angles are 3°. There are three shorter (2.03 Å) and three longer (2.53 Å) Ni–O bond lengths. In the second Ni+1.60+ site, Ni+1.60+ is bonded to four equivalent O2- atoms to form a mixture of corner and face-sharing NiO4 tetrahedra. The corner-sharing octahedral tilt angles are 53°. All Ni–O bond lengths are 2.15 Å. O2- is bonded in a 7-coordinate geometry to seven Ni+1.60+ atoms.
DOI: 10.17188/1662955
title: Materials Data on Ba3Sr(ClF)4 by Materials Project

description: Ba3Sr(ClF)4 crystallizes in the tetragonal P4mm space group. The structure is three-dimensional. there are three inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to five Cl1- and four equivalent F1- atoms. There are one shorter (3.27 Å) and four longer (3.30 Å) Ba–Cl bond lengths. All Ba–F bond lengths are 2.68 Å. In the second Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to five Cl1- and four equivalent F1- atoms. There are one shorter (3.22 Å) and four longer (3.31 Å) Ba–Cl bond lengths. All Ba–F bond lengths are 2.68 Å. In the third Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to five Cl1- and four equivalent F1- atoms. There are one shorter (3.24 Å) and four longer (3.29 Å) Ba–Cl bond lengths. All Ba–F bond lengths are 2.68 Å. Sr2+ is bonded in a 9-coordinate geometry to five Cl1- and four equivalent F1- atoms. There are one shorter (3.13 Å) and four longer (3.28 Å) Sr–Cl bond lengths. All Sr–F bond lengths are 2.57 Å. There are four inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 5-coordinate geometry to four equivalent Ba2+ and one Sr2+ atom. In the second Cl1- site, Cl1- is bonded in a 5-coordinate geometry to five Ba2+ atoms. In the third Cl1- site, Cl1- is bonded in a 1-coordinate geometry to one Ba2+, four equivalent Sr2+, and four equivalent F1- atoms. All Cl–F bond lengths are 3.25 Å. In the fourth Cl1- site, Cl1- is bonded in a 5-coordinate geometry to five Ba2+ atoms. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to four Ba2+ atoms to form a mixture of edge and corner-sharing FBa4 tetrahedra. In the second F1- site, F1- is bonded to two equivalent Ba2+, two equivalent Sr2+, and two equivalent Cl1- atoms to form a mixture of edge, face, and corner-sharing FBa2Sr2Cl2 tetrahedra.
DOI: 10.17188/1662956
title: Materials Data on PH11(C2Cl)2 by Materials Project

description: (C4PH11Cl)2Cl2 is Silicon tetrafluoride-derived structured and crystallizes in the orthorhombic Pbca space group. The structure is zero-dimensional and consists of eight hydrochloric acid molecules and eight schembl8954575 molecules.
DOI: 10.17188/1662957
title: Materials Data on HfZrOs2 by Materials Project

description: HfZrOs2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Hf is bonded in a body-centered cubic geometry to eight equivalent Os atoms. All Hf–Os bond lengths are 2.84 Å. Zr is bonded in a body-centered cubic geometry to eight equivalent Os atoms. All Zr–Os bond lengths are 2.84 Å. Os is bonded in a body-centered cubic geometry to four equivalent Hf and four equivalent Zr atoms.
DOI: 10.17188/1662959
title: Materials Data on PrCu3Pd2 by Materials Project

description: PrCu3Pd2 crystallizes in the orthorhombic Imm2 space group. The structure is three-dimensional. Pr is bonded in a 10-coordinate geometry to six equivalent Pd and ten Cu atoms. There are four shorter (3.02 Å) and two longer (3.03 Å) Pr–Pd bond lengths. There are a spread of Pr–Cu bond distances ranging from 3.06–3.27 Å. Pd is bonded to three equivalent Pr, two equivalent Pd, and seven Cu atoms to form a mixture of distorted corner, edge, and face-sharing PdPr3Cu7Pd2 cuboctahedra. There are one shorter (2.72 Å) and one longer (2.76 Å) Pd–Pd bond lengths. There are a spread of Pd–Cu bond distances ranging from 2.58–3.11 Å. There are two inequivalent Cu sites. In the first Cu site, Cu is bonded in a 12-coordinate geometry to three equivalent Pr, four equivalent Pd, and five Cu atoms. There are a spread of Cu–Cu bond distances ranging from 2.50–3.18 Å. In the second Cu site, Cu is bonded in a 12-coordinate geometry to four equivalent Pr, six equivalent Pd, and six equivalent Cu atoms.
DOI: 10.17188/1662960
title: Materials Data on VCdAgO4 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: 10.17188/1662961
title: Materials Data on LiV2F5 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: 10.17188/1662962
title: Materials Data on Ir(C2N3)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: 10.17188/1662963
title: Materials Data on GdAlNi by Materials Project

description: GdNiAl crystallizes in the orthorhombic Amm2 space group. The structure is three-dimensional. there are two inequivalent Gd sites. In the first Gd site, Gd is bonded in a 12-coordinate geometry to three equivalent Gd, five Ni, and seven Al atoms. There are two shorter (3.17 Å) and one longer (3.20 Å) Gd–Gd bond lengths. There are three shorter (2.88 Å) and two longer (3.12 Å) Gd–Ni bond lengths. There are a spread of Gd–Al bond distances ranging from 3.05–3.12 Å. In the second Gd site, Gd is bonded in a 12-coordinate geometry to four Gd, seven Ni, and five Al atoms. The Gd–Gd bond length is 2.91 Å. There are a spread of Gd–Ni bond distances ranging from 2.96–3.05 Å. There are a spread of Gd–Al bond distances ranging from 3.00–3.10 Å. There are three inequivalent Ni sites. In the first Ni site, Ni is bonded to six Gd and six Al atoms to form NiGd6Al6 cuboctahedra that share corners with four equivalent AlGd6Al2Ni4 cuboctahedra, corners with fourteen NiGd6Al6 cuboctahedra, edges with six NiGd6Al6 cuboctahedra, faces with four equivalent NiGd6Al2Ni4 cuboctahedra, and faces with fourteen AlGd6Al2Ni4 cuboctahedra. There are a spread of Ni–Al bond distances ranging from 2.57–2.65 Å. In the second Ni site, Ni is bonded to six Gd, four Ni, and two equivalent Al atoms to form distorted NiGd6Al2Ni4 cuboctahedra that share corners with eight NiGd6Al6 cuboctahedra, corners with ten AlGd6Al2Ni4 cuboctahedra, edges with two equivalent NiGd6Al2Ni4 cuboctahedra, edges with four equivalent AlGd6Al4Ni2 cuboctahedra, faces with eight AlGd6Al2Ni4 cuboctahedra, and faces with ten NiGd6Al6 cuboctahedra. There are a spread of Ni–Ni bond distances ranging from 2.60–2.63 Å. Both Ni–Al bond lengths are 2.49 Å. In the third Ni site, Ni is bonded to six Gd, four equivalent Ni, and two equivalent Al atoms to form distorted NiGd6Al2Ni4 cuboctahedra that share corners with six NiGd6Al6 cuboctahedra, corners with twelve AlGd6Al2Ni4 cuboctahedra, edges with six NiGd6Al6 cuboctahedra, faces with eight equivalent NiGd6Al2Ni4 cuboctahedra, and faces with ten AlGd6Al2Ni4 cuboctahedra. Both Ni–Al bond lengths are 2.49 Å. There are two inequivalent Al sites. In the first Al site, Al is bonded to six Gd, four Ni, and two equivalent Al atoms to form distorted AlGd6Al2Ni4 cuboctahedra that share corners with four equivalent AlGd6Al4Ni2 cuboctahedra, corners with eight NiGd6Al6 cuboctahedra, edges with six equivalent AlGd6Al2Ni4 cuboctahedra, faces with eight AlGd6Al2Ni4 cuboctahedra, and faces with twelve NiGd6Al6 cuboctahedra. Both Al–Al bond lengths are 2.66 Å. In the second Al site, Al is bonded to six Gd, two equivalent Ni, and four Al atoms to form distorted AlGd6Al4Ni2 cuboctahedra that share corners with eight AlGd6Al2Ni4 cuboctahedra, corners with ten NiGd6Al2Ni4 cuboctahedra, edges with two equivalent AlGd6Al4Ni2 cuboctahedra, edges with four equivalent NiGd6Al2Ni4 cuboctahedra, faces with eight NiGd6Al6 cuboctahedra, and faces with ten AlGd6Al2Ni4 cuboctahedra. There are one shorter (2.59 Å) and one longer (2.67 Å) Al–Al bond lengths.
DOI: 10.17188/1662964
title: Materials Data on Li2MnVP2(HO5)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: 10.17188/1662965
title: Materials Data on NaV3F10 by Materials Project

description: NaV3F10 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. Na1+ is bonded to eight F1- atoms to form distorted NaF8 hexagonal bipyramids that share corners with two equivalent VF6 octahedra and edges with six VF6 octahedra. The corner-sharing octahedral tilt angles are 8°. There are a spread of Na–F bond distances ranging from 2.13–2.86 Å. There are two inequivalent V3+ sites. In the first V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share corners with six equivalent VF6 octahedra and edges with two equivalent NaF8 hexagonal bipyramids. The corner-sharing octahedra tilt angles range from 1–34°. There are a spread of V–F bond distances ranging from 1.97–1.99 Å. In the second V3+ site, V3+ is bonded to six F1- atoms to form VF6 octahedra that share a cornercorner with one NaF8 hexagonal bipyramid, corners with five VF6 octahedra, and edges with two equivalent NaF8 hexagonal bipyramids. The corner-sharing octahedra tilt angles range from 1–36°. There are a spread of V–F bond distances ranging from 1.86–2.02 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a linear geometry to one Na1+ and one V3+ atom. In the second F1- site, F1- is bonded in a 2-coordinate geometry to one Na1+ and two equivalent V3+ atoms. In the third F1- site, F1- is bonded in a 2-coordinate geometry to one Na1+ and two V3+ atoms. In the fourth F1- site, F1- is bonded in a linear geometry to two V3+ atoms. In the fifth F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Na1+ and two V3+ atoms.
DOI: 10.17188/1662966
title: Materials Data on Zr3Bi by Materials Project

description: Zr3Bi crystallizes in the tetragonal I-4 space group. The structure is three-dimensional. there are three inequivalent Zr sites. In the first Zr site, Zr is bonded in a 3-coordinate geometry to three equivalent Bi atoms. There are a spread of Zr–Bi bond distances ranging from 2.97–3.15 Å. In the second Zr site, Zr is bonded in a distorted water-like geometry to two equivalent Bi atoms. There are one shorter (3.00 Å) and one longer (3.16 Å) Zr–Bi bond lengths. In the third Zr site, Zr is bonded in a 4-coordinate geometry to four equivalent Bi atoms. There are a spread of Zr–Bi bond distances ranging from 3.01–3.04 Å. Bi is bonded in a 9-coordinate geometry to nine Zr atoms.
DOI: 10.17188/1662967
title: Materials Data on CsK2SbF6 by Materials Project

description: (K)2CsSbF6 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional and consists of eight potassium molecules and one CsSbF6 framework. In the CsSbF6 framework, Cs1+ is bonded to six equivalent F1- atoms to form CsF6 octahedra that share corners with six equivalent SbF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Cs–F bond lengths are 2.80 Å. Sb3+ is bonded to six equivalent F1- atoms to form SbF6 octahedra that share corners with six equivalent CsF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sb–F bond lengths are 2.20 Å. F1- is bonded in a linear geometry to one Cs1+ and one Sb3+ atom.
DOI: 10.17188/1662970
title: Materials Data on Ba3UMnSe6 by Materials Project

description: Ba3UMnSe6 crystallizes in the trigonal R-3c space group. The structure is three-dimensional. Ba2+ is bonded in a 8-coordinate geometry to eight equivalent Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.33–3.46 Å. U4+ is bonded to six equivalent Se2- atoms to form distorted USe6 pentagonal pyramids that share faces with two equivalent MnSe6 octahedra. All U–Se bond lengths are 2.85 Å. Mn2+ is bonded to six equivalent Se2- atoms to form MnSe6 octahedra that share faces with two equivalent USe6 pentagonal pyramids. All Mn–Se bond lengths are 2.73 Å. Se2- is bonded to four equivalent Ba2+, one U4+, and one Mn2+ atom to form a mixture of distorted edge, face, and corner-sharing SeBa4UMn octahedra. The corner-sharing octahedra tilt angles range from 0–67°.
DOI: 10.17188/1662971
title: Materials Data on RhN5O7 by Materials Project

description: (RhNO)2N2(NO2)6 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four ammonia molecules, twelve nitrous acid molecules, and two RhNO clusters. In each RhNO cluster, Rh3+ is bonded in a distorted trigonal non-coplanar geometry to one N+2.20+ and two equivalent O2- atoms. The Rh–N bond length is 1.65 Å. There is one shorter (1.96 Å) and one longer (1.97 Å) Rh–O bond length. N+2.20+ is bonded in a single-bond geometry to one Rh3+ atom. O2- is bonded in a water-like geometry to two equivalent Rh3+ atoms.
DOI: 10.17188/1662972
title: Materials Data on K2UF6 by Materials Project

description: K2UF6 crystallizes in the orthorhombic Immm space group. The structure is three-dimensional. K1+ is bonded in a body-centered cubic geometry to eight F1- atoms. There are a spread of K–F bond distances ranging from 2.71–2.81 Å. U4+ is bonded in a body-centered cubic geometry to eight F1- atoms. There are four shorter (2.22 Å) and four longer (2.41 Å) U–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to three equivalent K1+ and one U4+ atom to form a mixture of distorted edge and corner-sharing FK3U tetrahedra. In the second F1- site, F1- is bonded to two equivalent K1+ and two equivalent U4+ atoms to form a mixture of distorted edge and corner-sharing FK2U2 tetrahedra.
DOI: 10.17188/1662973
title: Materials Data on SrYPt2 by Materials Project

description: SrYPt2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two SrYPt2 ribbons oriented in the (1, 0, 0) direction. Sr is bonded in a linear geometry to two equivalent Pt atoms. Both Sr–Pt bond lengths are 2.93 Å. Y is bonded in a linear geometry to two equivalent Pt atoms. Both Y–Pt bond lengths are 2.49 Å. Pt is bonded in a linear geometry to one Sr and one Y atom.