cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1694501
title: Materials Data on Mg(IO8)2 by Materials Project

description: MgO6(O5I)2 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of two magnesium;dihydroxide;tetrahydrate molecules and two O5I clusters. In each O5I cluster, there are five inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one I atom. The O–I bond length is 1.90 Å. In the second O site, O is bonded in a single-bond geometry to one I atom. The O–I bond length is 1.93 Å. In the third O site, O is bonded in a single-bond geometry to one I atom. The O–I bond length is 1.87 Å. In the fourth O site, O is bonded in a single-bond geometry to one I atom. The O–I bond length is 1.86 Å. In the fifth O site, O is bonded in a water-like geometry to two equivalent I atoms. There are one shorter (2.00 Å) and one longer (2.01 Å) O–I bond lengths. I is bonded to six O atoms to form edge-sharing IO6 octahedra.
DOI: 10.17188/1694502
title: Materials Data on Li2YIn by Materials Project

description: Li2YIn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Li2YIn ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to one Y and one In atom. The Li–Y bond length is 3.10 Å. The Li–In bond length is 2.84 Å. Y is bonded in a linear geometry to two equivalent Li atoms. In is bonded in a linear geometry to two equivalent Li atoms.
DOI: 10.17188/1694504
title: Materials Data on Li3FeO3 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: 10.17188/1694506
title: Materials Data on Li2Co3NiO8 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: 10.17188/1694507
title: Materials Data on GeCN2 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: 10.17188/1694508
title: Materials Data on Sr2NdMn2O7 by Materials Project

description: NdSr2Mn2O7 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.48–2.78 Å. Nd3+ is bonded to twelve O2- atoms to form NdO12 cuboctahedra that share corners with four equivalent NdO12 cuboctahedra, faces with four equivalent NdO12 cuboctahedra, and faces with eight equivalent MnO6 octahedra. There are eight shorter (2.67 Å) and four longer (2.77 Å) Nd–O bond lengths. Mn+3.50+ is bonded to six O2- atoms to form MnO6 octahedra that share corners with five equivalent MnO6 octahedra and faces with four equivalent NdO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–9°. There is one shorter (1.94 Å) and five longer (1.96 Å) Mn–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to five equivalent Sr2+ and one Mn+3.50+ atom to form a mixture of distorted corner and edge-sharing OSr5Mn octahedra. The corner-sharing octahedral tilt angles are 9°. In the second O2- site, O2- is bonded in a distorted linear geometry to two equivalent Sr2+, two equivalent Nd3+, and two equivalent Mn+3.50+ atoms. In the third O2- site, O2- is bonded in a distorted linear geometry to four equivalent Nd3+ and two equivalent Mn+3.50+ atoms.
DOI: 10.17188/1694509
title: Materials Data on Nd(Ni2Sn)2 by Materials Project

description: Nd(Ni2Sn)2 crystallizes in the tetragonal I4/mcm space group. The structure is three-dimensional. Nd is bonded in a 8-coordinate geometry to eight equivalent Ni and eight equivalent Sn atoms. All Nd–Ni bond lengths are 3.07 Å. All Nd–Sn bond lengths are 3.53 Å. Ni is bonded in a 10-coordinate geometry to two equivalent Nd, four equivalent Ni, and four equivalent Sn atoms. There are a spread of Ni–Ni bond distances ranging from 2.54–2.79 Å. There are a spread of Ni–Sn bond distances ranging from 2.58–2.68 Å. Sn is bonded in a 12-coordinate geometry to four equivalent Nd and eight equivalent Ni atoms.
DOI: 10.17188/1694510
title: Materials Data on Ni8Bi8SI2 by Materials Project

description: Ni8Bi8SI2 crystallizes in the orthorhombic P2_12_12 space group. The structure is three-dimensional. there are four inequivalent Ni sites. In the first Ni site, Ni is bonded in a distorted single-bond geometry to four Bi and one S atom. There are a spread of Ni–Bi bond distances ranging from 2.72–2.77 Å. The Ni–S bond length is 2.25 Å. In the second Ni site, Ni is bonded in a distorted single-bond geometry to four Bi and one S atom. There are a spread of Ni–Bi bond distances ranging from 2.72–2.75 Å. The Ni–S bond length is 2.30 Å. In the third Ni site, Ni is bonded in a distorted single-bond geometry to four Bi and one S atom. There are a spread of Ni–Bi bond distances ranging from 2.73–2.75 Å. The Ni–S bond length is 2.22 Å. In the fourth Ni site, Ni is bonded in a distorted single-bond geometry to four Bi and one S atom. There are a spread of Ni–Bi bond distances ranging from 2.72–2.75 Å. The Ni–S bond length is 2.28 Å. There are four inequivalent Bi sites. In the first Bi site, Bi is bonded in a 4-coordinate geometry to four Ni atoms. In the second Bi site, Bi is bonded in a 4-coordinate geometry to four Ni atoms. In the third Bi site, Bi is bonded in a 5-coordinate geometry to four Ni and one I atom. The Bi–I bond length is 3.56 Å. In the fourth Bi site, Bi is bonded in a 5-coordinate geometry to four Ni and one I atom. The Bi–I bond length is 3.51 Å. S is bonded in a 8-coordinate geometry to eight Ni atoms. I is bonded in a distorted linear geometry to two Bi atoms.
DOI: 10.17188/1694511
title: Materials Data on V7O13 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: 10.17188/1694512
title: Materials Data on Tm2ZnAu by Materials Project

description: Tm2AuZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Tm is bonded in a body-centered cubic geometry to four equivalent Au and four equivalent Zn atoms. All Tm–Au bond lengths are 3.07 Å. All Tm–Zn bond lengths are 3.07 Å. Au is bonded in a body-centered cubic geometry to eight equivalent Tm atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Tm atoms.
DOI: 10.17188/1694513
title: Materials Data on YAlPd2 by Materials Project

description: YPd2Al crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Y is bonded in a 8-coordinate geometry to eight equivalent Pd atoms. There are six shorter (2.98 Å) and two longer (3.02 Å) Y–Pd bond lengths. Pd is bonded in a 7-coordinate geometry to four equivalent Y and three equivalent Al atoms. All Pd–Al bond lengths are 2.63 Å. Al is bonded in a 6-coordinate geometry to six equivalent Pd atoms.
DOI: 10.17188/1694515
title: Materials Data on Na3CrP8O23 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: 10.17188/1694516
title: Materials Data on CsCrH8(NO4)2 by Materials Project

description: CsCrO8(NH4)2 crystallizes in the tetragonal I-42m space group. The structure is three-dimensional and consists of four ammonium molecules and one CsCrO8 framework. In the CsCrO8 framework, Cs1+ is bonded to eight O2- atoms to form distorted CsO8 hexagonal bipyramids that share corners with four equivalent CrO8 hexagonal bipyramids and edges with two equivalent CrO8 hexagonal bipyramids. There are four shorter (3.08 Å) and four longer (3.20 Å) Cs–O bond lengths. Cr5+ is bonded to eight O2- atoms to form distorted CrO8 hexagonal bipyramids that share corners with four equivalent CsO8 hexagonal bipyramids and edges with two equivalent CsO8 hexagonal bipyramids. There is four shorter (1.92 Å) and four longer (1.96 Å) Cr–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 1-coordinate geometry to one Cs1+, one Cr5+, and one O2- atom. The O–O bond length is 1.45 Å. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Cs1+, one Cr5+, and one O2- atom.
DOI: 10.17188/1694517
title: Materials Data on NbV3O8 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: 10.17188/1694518
title: Materials Data on Rb2NaAuCl6 by Materials Project

description: Rb2NaAuCl6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Rb1+ is bonded to twelve equivalent Cl1- atoms to form RbCl12 cuboctahedra that share corners with twelve equivalent RbCl12 cuboctahedra, faces with six equivalent RbCl12 cuboctahedra, faces with four equivalent NaCl6 octahedra, and faces with four equivalent AuCl6 octahedra. All Rb–Cl bond lengths are 3.73 Å. Na1+ is bonded to six equivalent Cl1- atoms to form NaCl6 octahedra that share corners with six equivalent AuCl6 octahedra and faces with eight equivalent RbCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Na–Cl bond lengths are 2.76 Å. Au3+ is bonded to six equivalent Cl1- atoms to form AuCl6 octahedra that share corners with six equivalent NaCl6 octahedra and faces with eight equivalent RbCl12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Au–Cl bond lengths are 2.52 Å. Cl1- is bonded in a distorted linear geometry to four equivalent Rb1+, one Na1+, and one Au3+ atom.
DOI: 10.17188/1694519
title: Materials Data on MnC4ClO4 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: 10.17188/1694520
title: Materials Data on FeH20C8NCl4 by Materials Project

description: (C2H5)4NFeCl4 crystallizes in the orthorhombic Pca2_1 space group. The structure is zero-dimensional and consists of four ethanaminium, n-ethyl-n,n-dimethyl- molecules; eight medicinal charcoal molecules; and four tetrachloroiron molecules.
DOI: 10.17188/1694521
title: Materials Data on Rb3Na(WO4)2 by Materials Project

description: Rb3Na(WO4)2 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. All Rb–O bond lengths are 3.14 Å. In the second Rb1+ site, Rb1+ is bonded in a 1-coordinate geometry to ten O2- atoms. There are a spread of Rb–O bond distances ranging from 2.65–3.38 Å. Na1+ is bonded to six equivalent O2- atoms to form NaO6 octahedra that share corners with six equivalent WO4 tetrahedra. All Na–O bond lengths are 2.51 Å. W6+ is bonded to four O2- atoms to form WO4 tetrahedra that share corners with three equivalent NaO6 octahedra. The corner-sharing octahedral tilt angles are 18°. There is one shorter (1.81 Å) and three longer (1.82 Å) W–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four Rb1+, one Na1+, and one W6+ atom. In the second O2- site, O2- is bonded in a linear geometry to one Rb1+ and one W6+ atom.
DOI: 10.17188/1694522
title: Materials Data on Mn3Ge by Materials Project

description: Mn3Ge crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Mn sites. In the first Mn site, Mn is bonded to nine Mn and three equivalent Ge atoms to form distorted MnMn9Ge3 cuboctahedra that share corners with six equivalent GeMn6 cuboctahedra, corners with twelve equivalent MnMn9Ge3 cuboctahedra, edges with six equivalent GeMn6 cuboctahedra, edges with eighteen MnMn9Ge3 cuboctahedra, and faces with twelve MnMn9Ge3 cuboctahedra. There are a spread of Mn–Mn bond distances ranging from 2.49–2.69 Å. There are two shorter (2.59 Å) and one longer (2.60 Å) Mn–Ge bond lengths. In the second Mn site, Mn is bonded to twelve Mn atoms to form MnMn12 cuboctahedra that share corners with six equivalent MnMn12 cuboctahedra, corners with six equivalent GeMn6 cuboctahedra, edges with six equivalent GeMn6 cuboctahedra, edges with eighteen MnMn9Ge3 cuboctahedra, and faces with eighteen MnMn9Ge3 cuboctahedra. There are four shorter (2.68 Å) and two longer (2.69 Å) Mn–Mn bond lengths. Ge is bonded to six equivalent Mn atoms to form distorted GeMn6 cuboctahedra that share corners with eighteen MnMn9Ge3 cuboctahedra, edges with six equivalent GeMn6 cuboctahedra, and edges with eighteen MnMn9Ge3 cuboctahedra.
DOI: 10.17188/1694523
title: Materials Data on CrI3 by Materials Project

description: CrI3 is Chromium trichloride structured and crystallizes in the trigonal P3_112 space group. The structure is two-dimensional and consists of three CrI3 sheets oriented in the (0, 0, 1) direction. Cr3+ is bonded to six I1- atoms to form edge-sharing CrI6 octahedra. There are four shorter (2.74 Å) and two longer (2.75 Å) Cr–I bond lengths. There are three inequivalent I1- sites. In the first I1- site, I1- is bonded in an L-shaped geometry to two equivalent Cr3+ atoms. In the second I1- site, I1- is bonded in an L-shaped geometry to two equivalent Cr3+ atoms. In the third I1- site, I1- is bonded in an L-shaped geometry to two equivalent Cr3+ atoms.
DOI: 10.17188/1694524
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: 10.17188/1694525
title: Materials Data on Dy4FeS7 by Materials Project

description: Dy4FeS7 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. there are four inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Dy–S bond distances ranging from 2.73–3.24 Å. In the second Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven S2- atoms. There are a spread of Dy–S bond distances ranging from 2.70–3.08 Å. In the third Dy3+ site, Dy3+ is bonded to six S2- atoms to form DyS6 octahedra that share a cornercorner with one DyS6 octahedra, a cornercorner with one FeS6 octahedra, and edges with two equivalent DyS6 octahedra. The corner-sharing octahedra tilt angles range from 44–52°. There are a spread of Dy–S bond distances ranging from 2.68–2.70 Å. In the fourth Dy3+ site, Dy3+ is bonded to six S2- atoms to form DyS6 octahedra that share a cornercorner with one DyS6 octahedra, corners with two equivalent FeS6 octahedra, edges with two equivalent DyS6 octahedra, and edges with three equivalent FeS6 octahedra. The corner-sharing octahedra tilt angles range from 9–44°. There are a spread of Dy–S bond distances ranging from 2.67–2.80 Å. Fe2+ is bonded to six S2- atoms to form FeS6 octahedra that share corners with three DyS6 octahedra, edges with two equivalent FeS6 octahedra, and edges with three equivalent DyS6 octahedra. The corner-sharing octahedra tilt angles range from 9–52°. There are a spread of Fe–S bond distances ranging from 2.34–2.47 Å. There are seven inequivalent S2- sites. In the first S2- site, S2- is bonded to four Dy3+ and one Fe2+ atom to form distorted SDy4Fe trigonal bipyramids that share corners with five SDy3Fe tetrahedra, edges with two equivalent SDy3Fe2 square pyramids, an edgeedge with one SDy4 tetrahedra, and edges with two equivalent SDy4Fe trigonal bipyramids. In the second S2- site, S2- is bonded to three Dy3+ and two equivalent Fe2+ atoms to form SDy3Fe2 square pyramids that share corners with five SDy3Fe tetrahedra, edges with two equivalent SDy3Fe2 square pyramids, an edgeedge with one SDy3Fe tetrahedra, and edges with two equivalent SDy4Fe trigonal bipyramids. In the third S2- site, S2- is bonded in a 5-coordinate geometry to five Dy3+ atoms. In the fourth S2- site, S2- is bonded in a 5-coordinate geometry to five Dy3+ atoms. In the fifth S2- site, S2- is bonded to three Dy3+ and one Fe2+ atom to form distorted SDy3Fe tetrahedra that share corners with four equivalent SDy3Fe2 square pyramids, corners with three SDy3Fe tetrahedra, a cornercorner with one SDy4Fe trigonal bipyramid, and an edgeedge with one SDy3Fe2 square pyramid. In the sixth S2- site, S2- is bonded to four Dy3+ atoms to form distorted SDy4 tetrahedra that share a cornercorner with one SDy3Fe2 square pyramid, corners with three SDy3Fe tetrahedra, corners with four equivalent SDy4Fe trigonal bipyramids, and an edgeedge with one SDy4Fe trigonal bipyramid. In the seventh S2- site, S2- is bonded in a rectangular see-saw-like geometry to two equivalent Dy3+ and two equivalent Fe2+ atoms.
DOI: 10.17188/1694526
title: Materials Data on Hf3Ga3Pd2Pt by Materials Project

description: Hf3PtPd2Ga3 crystallizes in the hexagonal P-6 space group. The structure is three-dimensional. there are two inequivalent Hf sites. In the first Hf site, Hf is bonded in a 11-coordinate geometry to two equivalent Pt, three Pd, and six equivalent Ga atoms. Both Hf–Pt bond lengths are 2.86 Å. There are two shorter (2.78 Å) and one longer (2.88 Å) Hf–Pd bond lengths. There are a spread of Hf–Ga bond distances ranging from 2.97–3.16 Å. In the second Hf site, Hf is bonded in a 11-coordinate geometry to two equivalent Pt, three Pd, and six equivalent Ga atoms. Both Hf–Pt bond lengths are 2.77 Å. There are two shorter (2.86 Å) and one longer (2.88 Å) Hf–Pd bond lengths. There are a spread of Hf–Ga bond distances ranging from 2.97–3.16 Å. Pt is bonded in a 9-coordinate geometry to six Hf and three equivalent Ga atoms. All Pt–Ga bond lengths are 2.69 Å. There are three inequivalent Pd sites. In the first Pd site, Pd is bonded in a 9-coordinate geometry to three equivalent Hf and six equivalent Ga atoms. All Pd–Ga bond lengths are 2.59 Å. In the second Pd site, Pd is bonded in a 9-coordinate geometry to three equivalent Hf and six equivalent Ga atoms. All Pd–Ga bond lengths are 2.58 Å. In the third Pd site, Pd is bonded in a 9-coordinate geometry to six Hf and three equivalent Ga atoms. All Pd–Ga bond lengths are 2.68 Å. Ga is bonded in a 10-coordinate geometry to six Hf, one Pt, and three Pd atoms.
DOI: 10.17188/1694527
title: Materials Data on RbSO2 by Materials Project

description: RbSO2 crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Rb is bonded in a 6-coordinate geometry to six equivalent O atoms. There are a spread of Rb–O bond distances ranging from 2.94–3.09 Å. S is bonded in a water-like geometry to two equivalent O atoms. Both S–O bond lengths are 1.53 Å. O is bonded in a 1-coordinate geometry to three equivalent Rb and one S atom.
DOI: 10.25403/upresearchdata.13668902
title: Regional cooperation and integration : intergovernmentalist approach to regional integration - a case of the AfCFTA

description: Regional cooperation and integration: case of the AfCFTA. The research study adopted qualitative methods, basically means it is qualitative.
DOI: 10.17188/1694529
title: Materials Data on Li3RhF6 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: 10.17188/1694530
title: Materials Data on Co3P4PbO14 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: 10.25403/upresearchdata.13668902.v1
title: Regional cooperation and integration : intergovernmentalist approach to regional integration - a case of the AfCFTA

description: Regional cooperation and integration: case of the AfCFTA. The research study adopted qualitative methods, basically means it is qualitative.
DOI: 10.17188/1694531
title: Materials Data on Ba3Sb2Se7 by Materials Project

description: Ba3Sb2Se7 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are three inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.35–3.51 Å. In the second Ba2+ site, Ba2+ is bonded in a 8-coordinate geometry to eight Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.33–3.54 Å. In the third Ba2+ site, Ba2+ is bonded in a 9-coordinate geometry to nine Se2- atoms. There are a spread of Ba–Se bond distances ranging from 3.38–3.58 Å. There are two inequivalent Sb4+ sites. In the first Sb4+ site, Sb4+ is bonded in a 3-coordinate geometry to three Se2- atoms. There are two shorter (2.60 Å) and one longer (2.68 Å) Sb–Se bond lengths. In the second Sb4+ site, Sb4+ is bonded in a 3-coordinate geometry to three Se2- atoms. There are a spread of Sb–Se bond distances ranging from 2.57–2.74 Å. There are seven inequivalent Se2- sites. In the first Se2- site, Se2- is bonded in a distorted see-saw-like geometry to three Ba2+ and one Sb4+ atom. In the second Se2- site, Se2- is bonded in a 6-coordinate geometry to four Ba2+ and one Se2- atom. The Se–Se bond length is 2.42 Å. In the third Se2- site, Se2- is bonded in a 1-coordinate geometry to two Ba2+, one Sb4+, and one Se2- atom. In the fourth Se2- site, Se2- is bonded in a 5-coordinate geometry to four Ba2+ and one Sb4+ atom. In the fifth Se2- site, Se2- is bonded to four Ba2+ and one Sb4+ atom to form a mixture of distorted edge, face, and corner-sharing SeBa4Sb square pyramids. In the sixth Se2- site, Se2- is bonded to four Ba2+ and one Sb4+ atom to form a mixture of distorted edge, face, and corner-sharing SeBa4Sb square pyramids. In the seventh Se2- site, Se2- is bonded to four Ba2+ and one Sb4+ atom to form a mixture of distorted edge, face, and corner-sharing SeBa4Sb square pyramids.
DOI: 10.17188/1694533
title: Materials Data on Al2TcPd by Materials Project

description: TcPdAl2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two TcPdAl2 ribbons oriented in the (1, 0, 0) direction. Tc is bonded in a linear geometry to two equivalent Al atoms. Both Tc–Al bond lengths are 2.42 Å. Pd is bonded in a linear geometry to two equivalent Al atoms. Both Pd–Al bond lengths are 2.39 Å. Al is bonded in a linear geometry to one Tc and one Pd atom.