cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.26050/wdcc/cxeu11dhr4
title: CORDEX simulation (evaluation) on 12.5 km grid over Europe based on RegCM4-2 (v1: MIT convection scheme) forced by ERA-Interim (EUR-11)

description: Project: CORDEX dynamical downscaling data sets based on CMIP5 forcing - CORDEX (http://wcrp-cordex.ipsl.jussieu.fr) is a WCRP initiative to coordinate the downscaling of CMIP5 simulation results produced in support of the IPCC/AR5. About 30 institutes worldwide contributed to the CORDEX data base with more than 20 RCMs in various configurations and versions. CORDEX defined 13 domains (http://wcrp-cordex.ipsl.jussieu.fr/images/pdf/cordex_regions.pdf) with acronyms AFR(Africa), EUR(Europe), ARC(Arctic), ANT(Antarctica), MED(Mediterranean), SAM(South America), CAM(Central America), NAM(North America), WAS(South Asia), EAS(East Asia), CAS(Central Asia), AUS(Austral-Asia), ARB(Mediterranean-North Africa). The priority domain is the African continent. The data are requested to be generated on model grids with an approximate grid cell distance of 50/25/12 km (acronyms -44/-22/-11), preferably on rotated regular latitude-longitude grids. A subset of the requested data is provided on 0.5/0.25/0.125° regular latitude/longitude grids in project CORDEX_DDS-CMIP5_lat-lon-grid. RCM evaluation with the ERA-Interim re-analyses data (1989-2008) is mandatory. Besides, downscaling of historical experiments (1950-2005) and of climate change scenarios RCP 4.5 and 8.5 is requested. Many groups also used RCP 2.6 climate projections. For more details see http://is-enes-data.github.io/cordex_archive_specifications.pdf . A list of the variables requested by CORDEX can be downloaded from this project (CORDEX_variables_requirement_table.pdf). Not all variables will be provided by all RCMs though. Note that 3 and 6 hourly data are also available, however, only at the modelling centres on request. Summary: This data of the project CORDEX includes CORDEX experiments for the domain for Europe in high resolution (EUR-11) based on DHMZ's RegCM4-2 model. Each file contains a single variable in the format NetCDF-4 compressed with CF standard names (CF-1.4). The data are provided on the model computational (native) grid. Information on additional project naming conventions is specified in the project description. The data include several daily, monthly and seasonal variables from the DHMZ-RegCM4-2 simulation forced by the ERA-Interim reanalysis. Data format follows CORDEX data protocol. Please contact ivan.guettler@cirus.dhz.hr for any relevant requests for this simulation.
DOI: 10.17188/1693353
title: Materials Data on Ce3Er by Materials Project

description: ErCe3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Er is bonded to twelve equivalent Ce atoms to form ErCe12 cuboctahedra that share corners with twelve equivalent ErCe12 cuboctahedra, edges with twenty-four equivalent CeCe8Er4 cuboctahedra, faces with six equivalent ErCe12 cuboctahedra, and faces with twelve equivalent CeCe8Er4 cuboctahedra. All Er–Ce bond lengths are 3.42 Å. Ce is bonded to four equivalent Er and eight equivalent Ce atoms to form CeCe8Er4 cuboctahedra that share corners with twelve equivalent CeCe8Er4 cuboctahedra, edges with eight equivalent ErCe12 cuboctahedra, edges with sixteen equivalent CeCe8Er4 cuboctahedra, faces with four equivalent ErCe12 cuboctahedra, and faces with fourteen equivalent CeCe8Er4 cuboctahedra. All Ce–Ce bond lengths are 3.42 Å.
DOI: 10.17188/1693354
title: Materials Data on BMoW by Materials Project

description: WMoB crystallizes in the orthorhombic Fmmm space group. The structure is three-dimensional. W is bonded in a 4-coordinate geometry to eight equivalent Mo and four equivalent B atoms. There are a spread of W–Mo bond distances ranging from 2.92–3.04 Å. All W–B bond lengths are 2.39 Å. Mo is bonded in a 4-coordinate geometry to eight equivalent W, three equivalent Mo, and four equivalent B atoms. There are one shorter (2.66 Å) and two longer (2.70 Å) Mo–Mo bond lengths. All Mo–B bond lengths are 2.40 Å. B is bonded in a 10-coordinate geometry to four equivalent W and four equivalent Mo atoms.
DOI: 10.17188/1693356
title: Materials Data on Na4Mg(GeSe3)2 by Materials Project

description: Na4Mg(GeSe3)2 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are four inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded to six Se2- atoms to form NaSe6 octahedra that share corners with six NaSe6 octahedra, edges with three equivalent MgSe6 octahedra, and edges with six NaSe6 octahedra. The corner-sharing octahedra tilt angles range from 6–13°. There are a spread of Na–Se bond distances ranging from 3.03–3.12 Å. In the second Na1+ site, Na1+ is bonded to six Se2- atoms to form NaSe6 octahedra that share corners with two equivalent NaSe6 octahedra, corners with two equivalent MgSe6 octahedra, edges with two equivalent MgSe6 octahedra, and edges with eight NaSe6 octahedra. The corner-sharing octahedra tilt angles range from 7–13°. There are a spread of Na–Se bond distances ranging from 3.05–3.16 Å. In the third Na1+ site, Na1+ is bonded to six Se2- atoms to form NaSe6 octahedra that share corners with two equivalent NaSe6 octahedra, corners with two equivalent MgSe6 octahedra, edges with two equivalent MgSe6 octahedra, and edges with eight NaSe6 octahedra. The corner-sharing octahedra tilt angles range from 6–7°. There are a spread of Na–Se bond distances ranging from 2.99–3.15 Å. In the fourth Na1+ site, Na1+ is bonded to six Se2- atoms to form NaSe6 octahedra that share corners with two equivalent NaSe6 octahedra, corners with two equivalent MgSe6 octahedra, edges with two equivalent MgSe6 octahedra, and edges with eight NaSe6 octahedra. The corner-sharing octahedra tilt angles range from 3–8°. There are a spread of Na–Se bond distances ranging from 2.97–3.05 Å. Mg2+ is bonded to six Se2- atoms to form MgSe6 octahedra that share corners with six NaSe6 octahedra and edges with nine NaSe6 octahedra. The corner-sharing octahedra tilt angles range from 3–7°. There are a spread of Mg–Se bond distances ranging from 2.79–2.86 Å. Ge3+ is bonded in a trigonal non-coplanar geometry to three Se2- atoms. There are two shorter (2.38 Å) and one longer (2.41 Å) Ge–Se bond lengths. There are three inequivalent Se2- sites. In the first Se2- site, Se2- is bonded to four Na1+, one Mg2+, and one Ge3+ atom to form a mixture of edge and corner-sharing SeNa4MgGe octahedra. The corner-sharing octahedra tilt angles range from 4–85°. In the second Se2- site, Se2- is bonded to four Na1+, one Mg2+, and one Ge3+ atom to form a mixture of edge and corner-sharing SeNa4MgGe octahedra. The corner-sharing octahedra tilt angles range from 4–85°. In the third Se2- site, Se2- is bonded to four Na1+, one Mg2+, and one Ge3+ atom to form a mixture of edge and corner-sharing SeNa4MgGe octahedra. The corner-sharing octahedra tilt angles range from 1–85°.
DOI: 10.17188/1693358
title: Materials Data on CrSbO4 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: 10.17188/1693359
title: Materials Data on HfBC by Materials Project

description: HfBC crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Hf is bonded to six equivalent B and six equivalent C atoms to form a mixture of face and edge-sharing HfB6C6 cuboctahedra. All Hf–B bond lengths are 2.54 Å. All Hf–C bond lengths are 2.54 Å. B is bonded in a trigonal planar geometry to six equivalent Hf and three equivalent C atoms. All B–C bond lengths are 1.70 Å. C is bonded in a distorted trigonal planar geometry to six equivalent Hf and three equivalent B atoms.
DOI: 10.17188/1693360
title: Materials Data on Am2(MoO4)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: 10.17188/1693361
title: Materials Data on Li2Si4(NiO4)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: 10.17188/1693364
title: Materials Data on K(InGa)2 by Materials Project

description: K(InGa)2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. K is bonded in a 8-coordinate geometry to eight equivalent In and eight equivalent Ga atoms. All K–In bond lengths are 3.80 Å. All K–Ga bond lengths are 3.63 Å. In is bonded to four equivalent K, four equivalent In, and four equivalent Ga atoms to form a mixture of distorted face, edge, and corner-sharing InK4In4Ga4 cuboctahedra. All In–In bond lengths are 3.39 Å. All In–Ga bond lengths are 2.91 Å. Ga is bonded in a 9-coordinate geometry to four equivalent K, four equivalent In, and one Ga atom. The Ga–Ga bond length is 2.58 Å.
DOI: 10.17188/1693365
title: Materials Data on Li5Nb2Co5O12 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: 10.17188/1693366
title: Materials Data on Yb(CoGe)6 by Materials Project

description: Yb(CoGe)6 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Yb is bonded to twelve equivalent Co and eight Ge atoms to form distorted YbCo12Ge8 hexagonal bipyramids that share faces with twenty-four equivalent CoYb2Co4Ge6 cuboctahedra and faces with six equivalent YbCo12Ge8 hexagonal bipyramids. All Yb–Co bond lengths are 3.21 Å. There are two shorter (2.68 Å) and six longer (2.93 Å) Yb–Ge bond lengths. Co is bonded to two equivalent Yb, four equivalent Co, and six Ge atoms to form distorted CoYb2Co4Ge6 cuboctahedra that share corners with fourteen equivalent CoYb2Co4Ge6 cuboctahedra, edges with seven equivalent CoYb2Co4Ge6 cuboctahedra, faces with nine equivalent CoYb2Co4Ge6 cuboctahedra, and faces with four equivalent YbCo12Ge8 hexagonal bipyramids. All Co–Co bond lengths are 2.54 Å. There are a spread of Co–Ge bond distances ranging from 2.44–2.64 Å. There are three inequivalent Ge sites. In the first Ge site, Ge is bonded in a 9-coordinate geometry to three equivalent Yb and six equivalent Co atoms. In the second Ge site, Ge is bonded in a 6-coordinate geometry to six equivalent Co atoms. In the third Ge site, Ge is bonded in a 8-coordinate geometry to one Yb, six equivalent Co, and one Ge atom. The Ge–Ge bond length is 2.47 Å.
DOI: 10.17188/1693367
title: Materials Data on Sr5(VN3)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: 10.17188/1693368
title: Materials Data on Li2Fe(CoO3)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: 10.25403/upresearchdata.13675555
title: Entrepreneurial resilience and success among women entrepreneurs in South Africa

description: Entrepreneurial activity has been widely associated with the growth of the economy, based on its ability to create employment and alleviate poverty. Entrepreneurs often function in uncertain environments and, as a result, require resilience in order to succeed. Research into entrepreneurial resilience, mainly in the field of positive psychology, is still at a preliminary stage. This study explores the relationship between resilience and success among women entrepreneurs in South Africa (SA). A narrative approach was employed to examine their journeys. Data was collected by means of semi-structured interviews of 16 respondents, across various provinces. Using qualitative thematic analysis, the researcher found that resilience is a precursor to entrepreneurial success. The results indicate resilience comes from a variety of influences, including situational factors, life experiences as well as adversity, and is influenced by factors including resourcefulness, optimism and hardiness. This trait therefore empowers an entrepreneur the ability to bounce back from business adversities and become successful; where success has been regarded as making a social impact. This study makes recommendations for entrepreneurs, business training institutions and incubators, as well as policy makers. <b></b>
DOI: 10.25387/g3.13003700
title: Supplemental Material for Nelson, et al., 2020

description: Genotypic, pedigree and phenotypic data
DOI: 10.17188/1693369
title: Materials Data on LiMnO2 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: 10.25387/g3.13003700.v1
title: Supplemental Material for Nelson, et al., 2020

description: Genotypic, pedigree and phenotypic data
DOI: 10.17188/1693370
title: Materials Data on Sm3Cu3Sb4 by Materials Project

description: Sm3Cu3Sb4 crystallizes in the cubic I-43d space group. The structure is three-dimensional. Sm3+ is bonded in a 8-coordinate geometry to eight equivalent Sb3- atoms. There are four shorter (3.32 Å) and four longer (3.40 Å) Sm–Sb bond lengths. Cu1+ is bonded in a 4-coordinate geometry to four equivalent Sb3- atoms. All Cu–Sb bond lengths are 2.70 Å. Sb3- is bonded in a 9-coordinate geometry to six equivalent Sm3+ and three equivalent Cu1+ atoms.
DOI: 10.17188/1693371
title: Materials Data on Tm5Ge3C by Materials Project

description: Tm5Ge3C crystallizes in the hexagonal P6_3/mcm space group. The structure is three-dimensional. there are two inequivalent Tm sites. In the first Tm site, Tm is bonded in a 6-coordinate geometry to six equivalent Ge atoms. All Tm–Ge bond lengths are 3.01 Å. In the second Tm site, Tm is bonded in a 2-coordinate geometry to five equivalent Ge and two equivalent C atoms. There are a spread of Tm–Ge bond distances ranging from 2.95–3.50 Å. Both Tm–C bond lengths are 2.44 Å. Ge is bonded in a 9-coordinate geometry to nine Tm atoms. C is bonded to six equivalent Tm atoms to form face-sharing CTm6 octahedra.
DOI: 10.6084/m9.figshare.13591208
title: Intention Survey Data.xlsx

description: Results of intention / self-efficacy survey regarding LTBI tx with 3HP for PLHIV in Uganda
DOI: 10.17188/1693372
title: Materials Data on Mn3Cr3O8 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: 10.17188/1693373
title: Materials Data on Ba5Mn3ClO12 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: 10.17188/1693374
title: Materials Data on Cu2P2O7 by Materials Project

description: Cu2P2O7 crystallizes in the monoclinic C2 space group. The structure is three-dimensional. there are two inequivalent Cu2+ sites. In the first Cu2+ site, Cu2+ is bonded in a 4-coordinate geometry to four O2- atoms. There is two shorter (1.94 Å) and two longer (2.01 Å) Cu–O bond length. In the second Cu2+ site, Cu2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Cu–O bond distances ranging from 1.93–2.61 Å. P5+ is bonded to four O2- atoms to form corner-sharing PO4 tetrahedra. There are a spread of P–O bond distances ranging from 1.52–1.59 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cu2+ and one P5+ atom. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two Cu2+ and one P5+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Cu2+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent P5+ atoms.
DOI: 10.17188/1693375
title: Materials Data on Ni4GePt5 by Materials Project

description: Pt5Ni4Ge crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are three inequivalent Pt2- sites. In the first Pt2- site, Pt2- is bonded to four equivalent Ni2+ and four equivalent Ge2+ atoms to form a mixture of distorted face, edge, and corner-sharing PtNi4Ge4 cuboctahedra. All Pt–Ni bond lengths are 2.68 Å. All Pt–Ge bond lengths are 2.67 Å. In the second Pt2- site, Pt2- is bonded in a distorted body-centered cubic geometry to eight Ni2+ atoms. There are four shorter (2.63 Å) and four longer (2.65 Å) Pt–Ni bond lengths. In the third Pt2- site, Pt2- is bonded to eight equivalent Ni2+ atoms to form a mixture of distorted face and edge-sharing PtNi8 cuboctahedra. All Pt–Ni bond lengths are 2.66 Å. There are two inequivalent Ni2+ sites. In the first Ni2+ site, Ni2+ is bonded in a body-centered cubic geometry to eight Pt2- atoms. In the second Ni2+ site, Ni2+ is bonded in a body-centered cubic geometry to eight Pt2- atoms. Ge2+ is bonded in a body-centered cubic geometry to eight equivalent Pt2- atoms.
DOI: 10.17188/1693376
title: Materials Data on MgSO6 by Materials Project

description: MgSO4O2 is Low Tridymite-derived structured and crystallizes in the orthorhombic P2_12_12_1 space group. The structure is three-dimensional and consists of eight hydrogen peroxide molecules and one MgSO4 framework. In the MgSO4 framework, there are two inequivalent Mg sites. In the first Mg site, Mg is bonded to four O atoms to form MgO4 tetrahedra that share corners with four SO4 tetrahedra. There is one shorter (1.95 Å) and three longer (1.96 Å) Mg–O bond length. In the second Mg site, Mg is bonded to four O atoms to form MgO4 tetrahedra that share corners with four SO4 tetrahedra. There are a spread of Mg–O bond distances ranging from 1.94–1.97 Å. There are two inequivalent S sites. In the first S site, S is bonded to four O atoms to form SO4 tetrahedra that share corners with four MgO4 tetrahedra. All S–O bond lengths are 1.48 Å. In the second S site, S is bonded to four O atoms to form SO4 tetrahedra that share corners with four MgO4 tetrahedra. All S–O bond lengths are 1.48 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom. In the second O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom. In the third O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom. In the fourth O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom. In the fifth O site, O is bonded in a linear geometry to one Mg and one S atom. In the sixth O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom. In the seventh O site, O is bonded in a linear geometry to one Mg and one S atom. In the eighth O site, O is bonded in a bent 150 degrees geometry to one Mg and one S atom.
DOI: 10.17188/1693378
title: Materials Data on Fe 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: 10.17188/1693380
title: Materials Data on Yb(NO4)3 by Materials Project

description: Yb(NO4)3 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two Yb(NO4)3 clusters. Yb is bonded in a 9-coordinate geometry to nine O atoms. There are a spread of Yb–O bond distances ranging from 2.44–2.55 Å. There are three inequivalent N sites. In the first N site, N is bonded in a trigonal planar geometry to three O atoms. There are a spread of N–O bond distances ranging from 1.24–1.28 Å. In the second N site, N is bonded in a trigonal planar geometry to three O atoms. There are a spread of N–O bond distances ranging from 1.24–1.28 Å. In the third N site, N is bonded in a trigonal planar geometry to three O atoms. There are a spread of N–O bond distances ranging from 1.23–1.27 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a distorted L-shaped geometry to one Yb and one N atom. In the second O site, O is bonded in a distorted L-shaped geometry to one Yb and one N atom. In the third O site, O is bonded in a distorted L-shaped geometry to one Yb and one N atom. In the fourth O site, O is bonded in a distorted water-like geometry to one Yb and one N atom. In the fifth O site, O is bonded in a distorted water-like geometry to one Yb and one N atom. In the sixth O site, O is bonded in a distorted water-like geometry to one Yb and one N atom. In the seventh O site, O is bonded in a single-bond geometry to one N atom. In the eighth O site, O is bonded in a single-bond geometry to one N atom. In the ninth O site, O is bonded in a single-bond geometry to one N atom. In the tenth O site, O is bonded in a single-bond geometry to one Yb atom. In the eleventh O site, O is bonded in a single-bond geometry to one Yb atom. In the twelfth O site, O is bonded in a single-bond geometry to one Yb atom.
DOI: 10.17188/1693381
title: Materials Data on YUCo10 by Materials Project

description: UYCo10 crystallizes in the orthorhombic Pmmm space group. The structure is three-dimensional. U is bonded in a distorted hexagonal planar geometry to eighteen Co atoms. There are a spread of U–Co bond distances ranging from 2.63–3.14 Å. Y is bonded in a 6-coordinate geometry to eighteen Co atoms. There are a spread of Y–Co bond distances ranging from 2.87–3.14 Å. There are five inequivalent Co sites. In the first Co site, Co is bonded in a 12-coordinate geometry to one U, two equivalent Y, and eight Co atoms. There are a spread of Co–Co bond distances ranging from 2.40–2.77 Å. In the second Co site, Co is bonded to two equivalent U, one Y, and nine Co atoms to form a mixture of distorted face, edge, and corner-sharing CoYU2Co9 cuboctahedra. There are a spread of Co–Co bond distances ranging from 2.37–2.57 Å. In the third Co site, Co is bonded to four equivalent U and eight Co atoms to form CoU4Co8 cuboctahedra that share corners with twenty-four CoY2U2Co8 cuboctahedra, edges with ten CoY2U2Co8 cuboctahedra, and faces with fourteen CoYU2Co9 cuboctahedra. All Co–Co bond lengths are 2.41 Å. In the fourth Co site, Co is bonded to four equivalent Y and eight Co atoms to form CoY4Co8 cuboctahedra that share corners with sixteen CoY2U2Co8 cuboctahedra, edges with ten CoY2U2Co8 cuboctahedra, and faces with eighteen CoYU2Co9 cuboctahedra. All Co–Co bond lengths are 2.42 Å. In the fifth Co site, Co is bonded to two equivalent U, two equivalent Y, and eight Co atoms to form CoY2U2Co8 cuboctahedra that share corners with twenty CoYU2Co9 cuboctahedra, edges with ten CoY2U2Co8 cuboctahedra, and faces with sixteen CoYU2Co9 cuboctahedra. There are one shorter (2.39 Å) and one longer (2.45 Å) Co–Co bond lengths.