cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.namsga
title: Occurrence Download

description: A dataset containing 20691 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Eriocheir sinensis H.Milne Edwards, 1853"
 ]
}

 The dataset includes 20691 records from 180 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0107395-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.s3352e
title: Occurrence Download

description: A dataset containing 1693 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is one of (China, Hong Kong, Macao, Chinese Taipei)",
 "TaxonKey is Anredera cordifolia (Ten.) Steenis"
 ]
}

 The dataset includes 1693 records from 21 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0107397-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.fn27jh
title: Occurrence Download

description: A dataset containing 966 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is one of (China, Hong Kong, Macao, Chinese Taipei)",
 "TaxonKey is Avena fatua L."
 ]
}

 The dataset includes 966 records from 38 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0107398-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15468/dl.xqqpdq
title: Occurrence Download

description: A dataset containing 7713 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Country is one of (Chinese Taipei, China, Hong Kong, Macao)",
 "TaxonKey is Bidens pilosa L."
 ]
}

 The dataset includes 7713 records from 64 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0107399-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.15148/dd520135-7656-4e80-91fe-f0284accbc76
title: A New Seismic Source Zone Model for Lesser Antilles Seismic Hazard Assessment - Data

description: Ouput data resulting from Foix et al. (2023) seismotectonic study as shapefiles and catalogs to be read and used by GIS software
DOI: 10.15468/dl.tawb5d
title: Occurrence Download

description: A dataset containing 221540 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Arabidopsis thaliana (L.) Heynh.)",
 "HasCoordinate is true",
 "HasGeospatialIssue is false"
 ]
}

 The dataset includes 221540 records from 1556 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0107387-240626123714530/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17188/1759358
title: Materials Data on Li2Mn3(BO3)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: 10.17188/1759359
title: Materials Data on BaYb3 by Materials Project

description: BaYb3 is beta Cu3Ti-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ba is bonded to twelve Yb atoms to form BaYb12 cuboctahedra that share corners with four equivalent BaYb12 cuboctahedra, corners with eight equivalent YbBa4Yb8 cuboctahedra, edges with eight equivalent BaYb12 cuboctahedra, edges with sixteen equivalent YbBa4Yb8 cuboctahedra, faces with four equivalent BaYb12 cuboctahedra, and faces with fourteen YbBa4Yb8 cuboctahedra. There are four shorter (4.03 Å) and eight longer (4.08 Å) Ba–Yb bond lengths. There are two inequivalent Yb sites. In the first Yb site, Yb is bonded to four equivalent Ba and eight Yb atoms to form YbBa4Yb8 cuboctahedra that share corners with twelve equivalent YbBa4Yb8 cuboctahedra, edges with eight equivalent BaYb12 cuboctahedra, edges with sixteen YbBa4Yb8 cuboctahedra, faces with four equivalent BaYb12 cuboctahedra, and faces with fourteen YbBa4Yb8 cuboctahedra. There are four shorter (4.03 Å) and four longer (4.08 Å) Yb–Yb bond lengths. In the second Yb site, Yb is bonded to four equivalent Ba and eight equivalent Yb atoms to form YbBa4Yb8 cuboctahedra that share corners with four equivalent YbBa4Yb8 cuboctahedra, corners with eight equivalent BaYb12 cuboctahedra, edges with twenty-four YbBa4Yb8 cuboctahedra, faces with six equivalent BaYb12 cuboctahedra, and faces with twelve YbBa4Yb8 cuboctahedra.
DOI: 10.17188/1759360
title: Materials Data on Sc3P by Materials Project

description: Sc3P is Cementite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. there are two inequivalent Sc sites. In the first Sc site, Sc is bonded in a 3-coordinate geometry to three equivalent P atoms. There are two shorter (2.69 Å) and one longer (2.85 Å) Sc–P bond lengths. In the second Sc site, Sc is bonded in a distorted bent 150 degrees geometry to two equivalent P atoms. There are one shorter (2.67 Å) and one longer (2.70 Å) Sc–P bond lengths. P is bonded in a 8-coordinate geometry to eight Sc atoms.
DOI: 10.17188/1759361
title: Materials Data on SrCa7Mn6Al2O21 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: 10.17188/1759363
title: Materials Data on LiFeSO4F by Materials Project

description: LiFeSO4F crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to four O2- and one F1- atom. There are a spread of Li–O bond distances ranging from 2.03–2.41 Å. The Li–F bond length is 1.88 Å. In the second Li1+ site, Li1+ is bonded in a 6-coordinate geometry to five O2- and one F1- atom. There are a spread of Li–O bond distances ranging from 2.11–2.75 Å. The Li–F bond length is 1.88 Å. There are two inequivalent Fe2+ sites. In the first Fe2+ site, Fe2+ is bonded to four O2- and two F1- atoms to form FeO4F2 octahedra that share corners with two equivalent FeO4F2 octahedra and corners with four SO4 tetrahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are a spread of Fe–O bond distances ranging from 2.11–2.23 Å. Both Fe–F bond lengths are 2.04 Å. In the second Fe2+ site, Fe2+ is bonded to four O2- and two F1- atoms to form FeO4F2 octahedra that share corners with two equivalent FeO4F2 octahedra and corners with four SO4 tetrahedra. The corner-sharing octahedra tilt angles range from 49–50°. There are a spread of Fe–O bond distances ranging from 2.14–2.22 Å. There are one shorter (2.03 Å) and one longer (2.04 Å) Fe–F bond lengths. There are two inequivalent S6+ sites. In the first S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with four FeO4F2 octahedra. The corner-sharing octahedra tilt angles range from 31–51°. There is two shorter (1.49 Å) and two longer (1.50 Å) S–O bond length. In the second S6+ site, S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with four FeO4F2 octahedra. The corner-sharing octahedra tilt angles range from 32–54°. There are a spread of S–O bond distances ranging from 1.48–1.50 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe2+, and one S6+ atom. In the third O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. In the fifth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. In the seventh O2- site, O2- is bonded in a distorted T-shaped geometry to one Li1+, one Fe2+, and one S6+ atom. In the eighth O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe2+, and one S6+ atom. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe2+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe2+ atoms.
DOI: 10.17188/1759364
title: Materials Data on V2OF5 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: 10.17188/1759365
title: Materials Data on Sr3Yb2O12 by Materials Project

description: Sr3Yb2O12 crystallizes in the cubic Ia-3d space group. The structure is three-dimensional. Sr is bonded to eight equivalent O atoms to form distorted edge-sharing SrO8 hexagonal bipyramids. There are four shorter (2.62 Å) and four longer (2.65 Å) Sr–O bond lengths. Yb is bonded in a hexagonal planar geometry to six equivalent O atoms. All Yb–O bond lengths are 2.24 Å. O is bonded in a trigonal non-coplanar geometry to two equivalent Sr and one Yb atom.
DOI: 10.17188/1759366
title: Materials Data on MnSO3 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: 10.17188/1759367
title: Materials Data on YAlN2 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: 10.17188/1759368
title: Materials Data on BaP3NO10 by Materials Project

description: BaP3NO10 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ba2+ is bonded to seven O2- atoms to form distorted BaO7 pentagonal bipyramids that share corners with six PO4 tetrahedra and an edgeedge with one BaO7 pentagonal bipyramid. There are a spread of Ba–O bond distances ranging from 2.62–2.89 Å. There are three inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with three equivalent BaO7 pentagonal bipyramids and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.48–1.68 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one BaO7 pentagonal bipyramid and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.47–1.71 Å. In the third P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent BaO7 pentagonal bipyramids and corners with two PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.48–1.70 Å. N3+ is bonded in a single-bond geometry to one O2- atom. The N–O bond length is 1.29 Å. There are ten inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Ba2+ and one P5+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two equivalent Ba2+ and one P5+ atom. In the third O2- site, O2- is bonded in a distorted single-bond geometry to one Ba2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a bent 120 degrees geometry to one P5+ and one N3+ atom. In the fifth O2- site, O2- is bonded in a distorted single-bond geometry to one Ba2+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the seventh O2- site, O2- is bonded in a distorted single-bond geometry to one Ba2+ and one P5+ atom. In the eighth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the ninth O2- site, O2- is bonded in a single-bond geometry to one Ba2+ atom. In the tenth O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms.
DOI: 10.17188/1759369
title: Materials Data on BaBeO3 by Materials Project

description: BaBeO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Ba is bonded to twelve equivalent O atoms to form BaO12 cuboctahedra that share corners with twelve equivalent BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, and faces with eight equivalent BeO6 octahedra. All Ba–O bond lengths are 2.75 Å. Be is bonded to six equivalent O atoms to form BeO6 octahedra that share corners with six equivalent BeO6 octahedra and faces with eight equivalent BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Be–O bond lengths are 1.95 Å. O is bonded in a distorted linear geometry to four equivalent Ba and two equivalent Be atoms.
DOI: 10.17188/1759370
title: Materials Data on Na5CrO4 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: 10.17188/1759372
title: Materials Data on Tb2Si3Pd by Materials Project

description: Tb2PdSi3 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Tb4+ sites. In the first Tb4+ site, Tb4+ is bonded to eight equivalent Si4- atoms to form TbSi8 hexagonal bipyramids that share corners with eight equivalent TbSi8 hexagonal bipyramids, edges with four equivalent TbSi12 cuboctahedra, edges with four equivalent TbSi8 hexagonal bipyramids, faces with two equivalent TbSi12 cuboctahedra, and faces with two equivalent TbSi8 hexagonal bipyramids. There are four shorter (3.06 Å) and four longer (3.16 Å) Tb–Si bond lengths. In the second Tb4+ site, Tb4+ is bonded to twelve equivalent Si4- atoms to form TbSi12 cuboctahedra that share edges with twelve equivalent TbSi8 hexagonal bipyramids, faces with two equivalent TbSi12 cuboctahedra, and faces with six equivalent TbSi8 hexagonal bipyramids. There are six shorter (3.07 Å) and six longer (3.09 Å) Tb–Si bond lengths. Pd4+ is bonded in a trigonal planar geometry to three equivalent Si4- atoms. All Pd–Si bond lengths are 2.41 Å. Si4- is bonded in a 1-coordinate geometry to six Tb4+, one Pd4+, and two equivalent Si4- atoms. Both Si–Si bond lengths are 2.36 Å.
DOI: 10.17188/1759373
title: Materials Data on ZnNiF6 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: 10.17188/1759374
title: Materials Data on Nb5Si3B by Materials Project

description: Nb5BSi3 crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. there are two inequivalent Nb3+ sites. In the first Nb3+ site, Nb3+ is bonded to six equivalent Si4- atoms to form distorted NbSi6 octahedra that share corners with six equivalent NbSi6 octahedra, corners with twelve equivalent NbSi5B2 pentagonal bipyramids, edges with three equivalent NbSi6 octahedra, faces with two equivalent NbSi6 octahedra, and faces with six equivalent NbSi5B2 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 33°. All Nb–Si bond lengths are 2.69 Å. In the second Nb3+ site, Nb3+ is bonded to two equivalent B3- and five equivalent Si4- atoms to form distorted NbSi5B2 pentagonal bipyramids that share corners with eight equivalent NbSi6 octahedra, corners with eight equivalent NbSi5B2 pentagonal bipyramids, edges with two equivalent NbSi5B2 pentagonal bipyramids, faces with four equivalent NbSi6 octahedra, and faces with six equivalent NbSi5B2 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 44–56°. Both Nb–B bond lengths are 2.31 Å. There are a spread of Nb–Si bond distances ranging from 2.69–2.91 Å. B3- is bonded to six equivalent Nb3+ atoms to form face-sharing BNb6 octahedra. Si4- is bonded in a 9-coordinate geometry to nine Nb3+ atoms.
DOI: 10.17188/1759377
title: Materials Data on Y2AlRu by Materials Project

description: Y2RuAl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Y2RuAl ribbons oriented in the (1, 0, 0) direction. Y is bonded in a linear geometry to one Ru and one Al atom. The Y–Ru bond length is 2.34 Å. The Y–Al bond length is 2.94 Å. Ru is bonded in a linear geometry to two equivalent Y atoms. Al is bonded in a linear geometry to two equivalent Y atoms.
DOI: 10.17188/1759378
title: Materials Data on GaNi3 by Materials Project

description: Ni3Ga is alpha bismuth trifluoride structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Ni sites. In the first Ni site, Ni is bonded to eight Ni and four equivalent Ga atoms to form distorted NiGa4Ni8 cuboctahedra that share corners with twelve equivalent NiGa4Ni8 cuboctahedra, edges with eight equivalent GaNi12 cuboctahedra, edges with sixteen NiGa4Ni8 cuboctahedra, faces with four equivalent GaNi12 cuboctahedra, and faces with fourteen NiGa4Ni8 cuboctahedra. There are four shorter (2.49 Å) and four longer (2.60 Å) Ni–Ni bond lengths. All Ni–Ga bond lengths are 2.49 Å. In the second Ni site, Ni is bonded to eight equivalent Ni and four equivalent Ga atoms to form NiGa4Ni8 cuboctahedra that share corners with four equivalent NiGa4Ni8 cuboctahedra, corners with eight equivalent GaNi12 cuboctahedra, edges with twenty-four NiGa4Ni8 cuboctahedra, faces with six equivalent GaNi12 cuboctahedra, and faces with twelve NiGa4Ni8 cuboctahedra. All Ni–Ga bond lengths are 2.60 Å. Ga is bonded to twelve Ni atoms to form GaNi12 cuboctahedra that share corners with four equivalent GaNi12 cuboctahedra, corners with eight equivalent NiGa4Ni8 cuboctahedra, edges with eight equivalent GaNi12 cuboctahedra, edges with sixteen equivalent NiGa4Ni8 cuboctahedra, faces with four equivalent GaNi12 cuboctahedra, and faces with fourteen NiGa4Ni8 cuboctahedra.
DOI: 10.17188/1759379
title: Materials Data on Sc2CdOs by Materials Project

description: Sc2OsCd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sc is bonded in a body-centered cubic geometry to four equivalent Os and four equivalent Cd atoms. All Sc–Os bond lengths are 2.91 Å. All Sc–Cd bond lengths are 2.91 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Cd is bonded in a distorted body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1759380
title: Materials Data on Mn2Al2O7 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: 10.17188/1759381
title: Materials Data on Cr2CoO4 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: 10.17188/1759383
title: Materials Data on Mg4CdAg5 by Materials Project

description: Mg4Ag5Cd is Heusler-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded in a body-centered cubic geometry to eight Ag atoms. There are four shorter (2.87 Å) and four longer (2.90 Å) Mg–Ag bond lengths. In the second Mg site, Mg is bonded in a body-centered cubic geometry to eight Ag atoms. There are four shorter (2.90 Å) and four longer (2.91 Å) Mg–Ag bond lengths. There are three inequivalent Ag sites. In the first Ag site, Ag is bonded in a body-centered cubic geometry to four equivalent Mg and four equivalent Cd atoms. All Ag–Cd bond lengths are 2.94 Å. In the second Ag site, Ag is bonded in a body-centered cubic geometry to eight Mg atoms. In the third Ag site, Ag is bonded in a body-centered cubic geometry to eight equivalent Mg atoms. Cd is bonded in a body-centered cubic geometry to eight equivalent Ag atoms.
DOI: 10.17188/1759384
title: Materials Data on Li2FeSi4O11 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: 10.17188/1759385
title: Materials Data on MgB12(H3O)12 by Materials Project

description: Mg(H2O)6(BH)12(H2O)6 crystallizes in the cubic F4_132 space group. The structure is zero-dimensional and consists of ninety-six boranediylradical molecules, eight magnesium;hexahydrate molecules, and forty-eight water molecules.
DOI: 10.17188/1759386
title: Materials Data on LiTe3 by Materials Project

description: LiTe3 crystallizes in the hexagonal P6_3/mmc space group. The structure is two-dimensional and consists of two LiTe3 sheets oriented in the (0, 0, 1) direction. Li is bonded in a hexagonal planar geometry to six equivalent Te atoms. All Li–Te bond lengths are 3.09 Å. Te is bonded in a distorted linear geometry to two equivalent Li atoms.