cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1751755
title: Materials Data on GaSiO3 by Materials Project

description: GaSiO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Ga2+ is bonded to twelve equivalent O2- atoms to form GaO12 cuboctahedra that share corners with twelve equivalent GaO12 cuboctahedra, faces with six equivalent GaO12 cuboctahedra, and faces with eight equivalent SiO6 octahedra. All Ga–O bond lengths are 2.53 Å. Si4+ is bonded to six equivalent O2- atoms to form SiO6 octahedra that share corners with six equivalent SiO6 octahedra and faces with eight equivalent GaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Si–O bond lengths are 1.79 Å. O2- is bonded in a distorted linear geometry to four equivalent Ga2+ and two equivalent Si4+ atoms.
DOI: 10.17188/1751756
title: Materials Data on Mg3Si4 by Materials Project

description: Mg3Si4 is Magnesium tetraboride-like structured and crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are six inequivalent Mg sites. In the first Mg site, Mg is bonded in a 4-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.79–3.24 Å. In the second Mg site, Mg is bonded in a 4-coordinate geometry to five Si atoms. There are a spread of Mg–Si bond distances ranging from 2.69–2.99 Å. In the third Mg site, Mg is bonded in a 4-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.73–3.31 Å. In the fourth Mg site, Mg is bonded in a 4-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.68–3.09 Å. In the fifth Mg site, Mg is bonded in a 5-coordinate geometry to five Si atoms. There are a spread of Mg–Si bond distances ranging from 2.66–2.95 Å. In the sixth Mg site, Mg is bonded in a 7-coordinate geometry to seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.67–3.15 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.46–2.48 Å. In the second Si site, Si is bonded in a 10-coordinate geometry to five Mg and five Si atoms. There are a spread of Si–Si bond distances ranging from 2.50–2.89 Å. In the third Si site, Si is bonded in a 8-coordinate geometry to five Mg and four Si atoms. There are one shorter (2.48 Å) and one longer (2.49 Å) Si–Si bond lengths. In the fourth Si site, Si is bonded in a 1-coordinate geometry to three Mg and three Si atoms. The Si–Si bond length is 2.66 Å. In the fifth Si site, Si is bonded in a 7-coordinate geometry to five Mg and two Si atoms. The Si–Si bond length is 2.51 Å. In the sixth Si site, Si is bonded in a 7-coordinate geometry to four Mg and three Si atoms. There are one shorter (2.52 Å) and one longer (2.58 Å) Si–Si bond lengths. In the seventh Si site, Si is bonded in a 7-coordinate geometry to four Mg and three Si atoms. In the eighth Si site, Si is bonded in a 9-coordinate geometry to six Mg and three Si atoms.
DOI: 10.17188/1751757
title: Materials Data on Li3FeP2HO8 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: 10.17188/1751758
title: Materials Data on HoAlNi4 by Materials Project

description: HoNi4Al crystallizes in the hexagonal P-6m2 space group. The structure is three-dimensional. Ho is bonded in a 6-coordinate geometry to fifteen Ni and three equivalent Al atoms. There are three shorter (2.90 Å) and twelve longer (3.16 Å) Ho–Ni bond lengths. All Ho–Al bond lengths are 2.90 Å. There are two inequivalent Ni sites. In the first Ni site, Ni is bonded to three equivalent Ho, six equivalent Ni, and three equivalent Al atoms to form NiHo3Al3Ni6 cuboctahedra that share corners with nine equivalent AlHo3Ni9 cuboctahedra, corners with twelve equivalent NiHo4Al2Ni6 cuboctahedra, edges with six equivalent NiHo3Al3Ni6 cuboctahedra, faces with three equivalent AlHo3Ni9 cuboctahedra, and faces with twenty NiHo3Al3Ni6 cuboctahedra. All Ni–Ni bond lengths are 2.40 Å. All Ni–Al bond lengths are 2.90 Å. In the second Ni site, Ni is bonded to four equivalent Ho, six Ni, and two equivalent Al atoms to form distorted NiHo4Al2Ni6 cuboctahedra that share corners with four equivalent AlHo3Ni9 cuboctahedra, corners with twenty NiHo3Al3Ni6 cuboctahedra, edges with ten equivalent NiHo4Al2Ni6 cuboctahedra, faces with six equivalent AlHo3Ni9 cuboctahedra, and faces with sixteen NiHo3Al3Ni6 cuboctahedra. There are two shorter (2.48 Å) and two longer (2.54 Å) Ni–Ni bond lengths. Both Ni–Al bond lengths are 2.42 Å. Al is bonded to three equivalent Ho and nine Ni atoms to form distorted AlHo3Ni9 cuboctahedra that share corners with twenty-one NiHo3Al3Ni6 cuboctahedra, edges with six equivalent AlHo3Ni9 cuboctahedra, faces with two equivalent AlHo3Ni9 cuboctahedra, and faces with twenty-one NiHo3Al3Ni6 cuboctahedra.
DOI: 10.17188/1751759
title: Materials Data on Ba20Cd4Hg99 by Materials Project

description: Ba20Hg99Cd4 crystallizes in the cubic F-43m space group. The structure is three-dimensional. there are four inequivalent Ba sites. In the first Ba site, Ba is bonded in a 6-coordinate geometry to eighteen Hg atoms. There are a spread of Ba–Hg bond distances ranging from 3.76–3.85 Å. In the second Ba site, Ba is bonded in a 11-coordinate geometry to seventeen Hg atoms. There are a spread of Ba–Hg bond distances ranging from 3.54–4.07 Å. In the third Ba site, Ba is bonded in a 1-coordinate geometry to fifteen Hg atoms. There are a spread of Ba–Hg bond distances ranging from 3.43–3.70 Å. In the fourth Ba site, Ba is bonded in a 12-coordinate geometry to sixteen Hg atoms. There are a spread of Ba–Hg bond distances ranging from 3.76–3.97 Å. There are twelve inequivalent Hg sites. In the first Hg site, Hg is bonded in a 7-coordinate geometry to four Ba and four Hg atoms. There are a spread of Hg–Hg bond distances ranging from 2.97–3.09 Å. In the second Hg site, Hg is bonded to three equivalent Ba and nine Hg atoms to form distorted face-sharing HgBa3Hg9 cuboctahedra. There are a spread of Hg–Hg bond distances ranging from 3.18–3.33 Å. In the third Hg site, Hg is bonded in a tetrahedral geometry to four equivalent Ba atoms. In the fourth Hg site, Hg is bonded in a distorted body-centered cubic geometry to four Ba, three Hg, and one Cd atom. The Hg–Hg bond length is 3.02 Å. The Hg–Cd bond length is 3.23 Å. In the fifth Hg site, Hg is bonded in a distorted q6 geometry to three equivalent Ba and six Hg atoms. There are three shorter (3.15 Å) and three longer (3.20 Å) Hg–Hg bond lengths. In the sixth Hg site, Hg is bonded in a 7-coordinate geometry to three equivalent Ba, three equivalent Hg, and one Cd atom. All Hg–Hg bond lengths are 3.10 Å. The Hg–Cd bond length is 3.14 Å. In the seventh Hg site, Hg is bonded in a 10-coordinate geometry to four Ba and six Hg atoms. In the eighth Hg site, Hg is bonded in a 10-coordinate geometry to two Ba and eight Hg atoms. There are two shorter (3.18 Å) and two longer (3.36 Å) Hg–Hg bond lengths. In the ninth Hg site, Hg is bonded in a 1-coordinate geometry to three Ba, three Hg, and one Cd atom. The Hg–Cd bond length is 2.93 Å. In the tenth Hg site, Hg is bonded in a distorted trigonal planar geometry to three Ba atoms. In the eleventh Hg site, Hg is bonded in a 8-coordinate geometry to three Ba and five Hg atoms. There are one shorter (2.98 Å) and two longer (3.04 Å) Hg–Hg bond lengths. In the twelfth Hg site, Hg is bonded in a 1-coordinate geometry to three equivalent Ba, three equivalent Hg, and one Cd atom. The Hg–Cd bond length is 3.25 Å. Cd is bonded in a body-centered cubic geometry to eight Hg atoms.
DOI: 10.17188/1751760
title: Materials Data on Mn2Co2SiGe by Materials Project

description: Mn2Co2GeSi crystallizes in the orthorhombic Pmc2_1 space group. The structure is three-dimensional. there are two inequivalent Mn sites. In the first Mn site, Mn is bonded in a 5-coordinate geometry to six Co, four equivalent Ge, and one Si atom. There are a spread of Mn–Co bond distances ranging from 2.70–2.85 Å. There are two shorter (2.56 Å) and two longer (2.60 Å) Mn–Ge bond lengths. The Mn–Si bond length is 2.52 Å. In the second Mn site, Mn is bonded in a 11-coordinate geometry to six Co, one Ge, and four equivalent Si atoms. There are a spread of Mn–Co bond distances ranging from 2.65–2.78 Å. The Mn–Ge bond length is 2.57 Å. There are two shorter (2.54 Å) and two longer (2.57 Å) Mn–Si bond lengths. There are two inequivalent Co sites. In the first Co site, Co is bonded in a 12-coordinate geometry to six Mn, two equivalent Co, two equivalent Ge, and two equivalent Si atoms. Both Co–Co bond lengths are 2.74 Å. Both Co–Ge bond lengths are 2.32 Å. There are one shorter (2.25 Å) and one longer (2.26 Å) Co–Si bond lengths. In the second Co site, Co is bonded in a 12-coordinate geometry to six Mn, two equivalent Co, two equivalent Ge, and two equivalent Si atoms. There are one shorter (2.35 Å) and one longer (2.37 Å) Co–Ge bond lengths. Both Co–Si bond lengths are 2.26 Å. Ge is bonded in a 9-coordinate geometry to five Mn and four Co atoms. Si is bonded in a 9-coordinate geometry to five Mn and four Co atoms.
DOI: 10.17188/1751761
title: Materials Data on Fe3(OF2)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: 10.17188/1751762
title: Materials Data on Li6MnV3(PO4)6 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: 10.17188/1751763
title: Materials Data on In3(GaN2)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: 10.17188/1751764
title: Materials Data on KPO4 by Materials Project

description: KPO4 crystallizes in the tetragonal I-42d space group. The structure is one-dimensional and consists of four KPO4 ribbons oriented in the (0, 0, 1) direction. K is bonded in a 4-coordinate geometry to four equivalent O atoms. All K–O bond lengths are 2.67 Å. P is bonded in a distorted tetrahedral geometry to four equivalent O atoms. All P–O bond lengths are 1.56 Å. O is bonded in a distorted water-like geometry to one K and one P atom.
DOI: 10.17188/1751766
title: Materials Data on Cs2LiPdF6 by Materials Project

description: Cs2LiPdF6 is (Cubic) Perovskite-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Cs is bonded to twelve equivalent F atoms to form CsF12 cuboctahedra that share corners with twelve equivalent CsF12 cuboctahedra, faces with six equivalent CsF12 cuboctahedra, faces with four equivalent LiF6 octahedra, and faces with four equivalent PdF6 octahedra. All Cs–F bond lengths are 3.09 Å. Li is bonded to six equivalent F atoms to form LiF6 octahedra that share corners with six equivalent PdF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Li–F bond lengths are 2.28 Å. Pd is bonded to six equivalent F atoms to form PdF6 octahedra that share corners with six equivalent LiF6 octahedra and faces with eight equivalent CsF12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Pd–F bond lengths are 2.09 Å. F is bonded in a distorted linear geometry to four equivalent Cs, one Li, and one Pd atom.
DOI: 10.17188/1751767
title: Materials Data on Ti(PbN)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: 10.17188/1751768
title: Materials Data on Rb4Zn(MoO4)3 by Materials Project

description: Rb4Zn(MoO4)3 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. there are four inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Rb–O bond distances ranging from 2.92–3.43 Å. In the second Rb1+ site, Rb1+ is bonded in a 7-coordinate geometry to nine O2- atoms. There are a spread of Rb–O bond distances ranging from 2.88–3.60 Å. In the third Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Rb–O bond distances ranging from 2.87–3.55 Å. In the fourth Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Rb–O bond distances ranging from 2.93–3.42 Å. There are three inequivalent Mo6+ sites. In the first Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share corners with two equivalent ZnO4 tetrahedra. There are a spread of Mo–O bond distances ranging from 1.77–1.84 Å. In the second Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share a cornercorner with one ZnO4 tetrahedra. There are a spread of Mo–O bond distances ranging from 1.78–1.85 Å. In the third Mo6+ site, Mo6+ is bonded to four O2- atoms to form MoO4 tetrahedra that share a cornercorner with one ZnO4 tetrahedra. There are a spread of Mo–O bond distances ranging from 1.78–1.84 Å. Zn2+ is bonded to four O2- atoms to form ZnO4 tetrahedra that share corners with four MoO4 tetrahedra. There are a spread of Zn–O bond distances ranging from 1.93–2.03 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one Mo6+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one Mo6+ atom. In the third O2- site, O2- is bonded in a 1-coordinate geometry to four Rb1+ and one Mo6+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one Mo6+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Rb1+, one Mo6+, and one Zn2+ atom. In the sixth O2- site, O2- is bonded in a distorted linear geometry to two Rb1+, one Mo6+, and one Zn2+ atom. In the seventh O2- site, O2- is bonded in a 1-coordinate geometry to three Rb1+ and one Mo6+ atom. In the eighth O2- site, O2- is bonded in a distorted single-bond geometry to four Rb1+ and one Mo6+ atom. In the ninth O2- site, O2- is bonded in a 3-coordinate geometry to two Rb1+ and one Mo6+ atom. In the tenth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Rb1+, one Mo6+, and one Zn2+ atom. In the eleventh O2- site, O2- is bonded in a 1-coordinate geometry to four Rb1+ and one Mo6+ atom. In the twelfth O2- site, O2- is bonded in a distorted bent 120 degrees geometry to two Rb1+, one Mo6+, and one Zn2+ atom.
DOI: 10.17188/1751769
title: Materials Data on Fe3OF7 by Materials Project

description: Fe3OF7 crystallizes in the monoclinic Cc space group. The structure is three-dimensional. there are three inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.94 Å. There are a spread of Fe–F bond distances ranging from 1.98–2.10 Å. In the second Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.99 Å. There are a spread of Fe–F bond distances ranging from 1.94–2.20 Å. In the third Fe3+ site, Fe3+ is bonded to one O2- and five F1- atoms to form edge-sharing FeOF5 octahedra. The Fe–O bond length is 1.95 Å. There are a spread of Fe–F bond distances ranging from 1.97–2.11 Å. O2- is bonded in a 3-coordinate geometry to three Fe3+ atoms. There are seven inequivalent F1- sites. In the first F1- site, F1- is bonded in an L-shaped geometry to two Fe3+ atoms. In the second F1- site, F1- is bonded in an L-shaped geometry to two Fe3+ atoms. In the third F1- site, F1- is bonded in a 3-coordinate geometry to three Fe3+ atoms. In the fourth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the fifth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the sixth F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms. In the seventh F1- site, F1- is bonded in a water-like geometry to two Fe3+ atoms.
DOI: 10.17188/1751770
title: Materials Data on FeBiPPbO7 by Materials Project

description: FePbBiPO7 crystallizes in the monoclinic Cm space group. The structure is three-dimensional. Fe2+ is bonded to six O2- atoms to form distorted FeO6 pentagonal pyramids that share a cornercorner with one BiO6 pentagonal pyramid, corners with two equivalent FeO6 pentagonal pyramids, corners with two equivalent PO4 tetrahedra, and edges with two equivalent BiO6 pentagonal pyramids. There are a spread of Fe–O bond distances ranging from 1.94–2.21 Å. Pb4+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Pb–O bond distances ranging from 2.41–2.76 Å. Bi3+ is bonded to six O2- atoms to form distorted BiO6 pentagonal pyramids that share a cornercorner with one FeO6 pentagonal pyramid, corners with two equivalent PO4 tetrahedra, edges with two equivalent FeO6 pentagonal pyramids, and edges with two equivalent BiO6 pentagonal pyramids. There are a spread of Bi–O bond distances ranging from 2.21–2.79 Å. P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent FeO6 pentagonal pyramids and corners with two equivalent BiO6 pentagonal pyramids. There are a spread of P–O bond distances ranging from 1.51–1.59 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to one Fe2+, two equivalent Pb4+, and one Bi3+ atom. In the second O2- site, O2- is bonded to one Fe2+, one Pb4+, and two equivalent Bi3+ atoms to form distorted corner-sharing OFeBi2Pb tetrahedra. In the third O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Pb4+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Bi3+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to two equivalent Fe2+ and one Bi3+ atom. In the sixth O2- site, O2- is bonded in a 2-coordinate geometry to one Fe2+, one Pb4+, and one P5+ atom.
DOI: 10.17188/1751771
title: Materials Data on Ba2AlCo2F11 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: 10.17188/1751772
title: Materials Data on Li2MnP2O7 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: 10.17188/1751773
title: Materials Data on Ba5Y8Mn4O21 by Materials Project

description: Ba5Y8Mn4O21 crystallizes in the tetragonal I4/m space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a distorted q6 geometry to ten O2- atoms. There are two shorter (2.91 Å) and eight longer (2.96 Å) Ba–O bond lengths. In the second Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten O2- atoms. There are a spread of Ba–O bond distances ranging from 2.67–3.30 Å. There are two inequivalent Y3+ sites. In the first Y3+ site, Y3+ is bonded to seven O2- atoms to form distorted YO7 pentagonal bipyramids that share corners with two equivalent YO7 pentagonal bipyramids, corners with two equivalent MnO5 trigonal bipyramids, edges with five YO7 pentagonal bipyramids, an edgeedge with one MnO5 trigonal bipyramid, and a faceface with one MnO5 trigonal bipyramid. There are a spread of Y–O bond distances ranging from 2.29–2.54 Å. In the second Y3+ site, Y3+ is bonded to seven O2- atoms to form distorted YO7 pentagonal bipyramids that share corners with three YO7 pentagonal bipyramids, corners with two equivalent MnO5 trigonal bipyramids, edges with three equivalent YO7 pentagonal bipyramids, edges with two equivalent MnO5 trigonal bipyramids, and faces with two equivalent YO7 pentagonal bipyramids. There are a spread of Y–O bond distances ranging from 2.30–2.47 Å. Mn2+ is bonded to five O2- atoms to form MnO5 trigonal bipyramids that share corners with four YO7 pentagonal bipyramids, edges with three YO7 pentagonal bipyramids, and a faceface with one YO7 pentagonal bipyramid. There are a spread of Mn–O bond distances ranging from 2.07–2.16 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Ba2+ and four equivalent Y3+ atoms to form distorted corner-sharing OBa2Y4 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second O2- site, O2- is bonded to four equivalent Ba2+, one Y3+, and one Mn2+ atom to form a mixture of distorted edge and corner-sharing OBa4YMn octahedra. The corner-sharing octahedral tilt angles are 7°. In the third O2- site, O2- is bonded in a 6-coordinate geometry to two Ba2+, three Y3+, and one Mn2+ atom. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ba2+, three Y3+, and one Mn2+ atom.
DOI: 10.17188/1751775
title: Materials Data on SrCa7TiMn7O24 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: 10.17188/1751776
title: Materials Data on PtN4Cl5O by Materials Project

description: (PtCl3)2N2(NO)2(NCl)4 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four ammonia molecules, eight chloramine molecules, four nitroxyl molecules, and four trichloroplatinum molecules.
DOI: 10.5281/zenodo.4499541
title: PR Rejection Reasons -- Hexo and ESLint Case Studies

description: A dataset of manually annotated pull request rejection reasons. Target projects: Hexo and ESLint (hosted on GitHub).