cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.6084/m9.figshare.21520857.v1
title: Propagule pressure samples

description: These fsc files contain the bacterial density estimates used to determine the propagule pressure needed to invade the lake water with Flavobacterium columnare.
DOI: 10.3886/e190861
title: Should the US federal government expand its efforts to help the poor

description: Even when controlling for big versus small government philosophies, this paper reports quantitatively significant cleavages in the probabilities of supporting increased federal antipoverty efforts persist between conservatives and liberals, and Republicans and Democrats. However, predicted conditional probabilities show that support for increased welfare spending or federal responsibility in raising the standard of living of the poor is not overwhelming, even among liberals and Democrats while support for increased federal assistance to the poor is fairly strong, even among conservatives and Republicans. Hence, we consider assertions that conservatives and Republicans do not care about the poor to be extreme and unsupported.<br>
DOI: 10.3886/e190861v1
title: Should the US federal government expand its efforts to help the poor

description: Even when controlling for big versus small government philosophies, this paper reports quantitatively significant cleavages in the probabilities of supporting increased federal antipoverty efforts persist between conservatives and liberals, and Republicans and Democrats. However, predicted conditional probabilities show that support for increased welfare spending or federal responsibility in raising the standard of living of the poor is not overwhelming, even among liberals and Democrats while support for increased federal assistance to the poor is fairly strong, even among conservatives and Republicans. Hence, we consider assertions that conservatives and Republicans do not care about the poor to be extreme and unsupported.<br>
DOI: 10.34740/kaggle/dsv/5603042
title: Nigerian Presidential Election 2023 Tweets
DOI: 10.5281/zenodo.7897038
title: Genome-wide association statistics of Hearing Problems

description: Genome-wide Association Statistics of Hearing Problems Citation: De Angelis F, Zeleznik OA, Wendt FR, Pathak GA, Tylee DS, De Lillo A, Koller D, Cabrera-Mendoza B, Clifford RE, Maihofer AX, Nievergelt CM, Curhan GC, Curhan SG, Polimanti R. Sex differences in the polygenic architecture of hearing problems in adults. Genome Med. https://doi.org/10.1186/s13073-023-01186-3 COLUMN HEADERS<br> chromosome: chromosome<br> base_pair_location: position<br> effect_allele: effect allele (corresponds to the effect size’s sign; may not be the alternate allele)<br> other_allele: non-effect allele<br> beta: effect measured as beta, sign corresponds to the effect of the effect allele<br> standard_error: standard error of the effect<br> effect_allele_frequency: effect allele frequency in UK Biobank participants of European descent<br> p_value: p value of the association statistic<br> variant_id: variant identifier<br> rs_id: rsID of the variant<br> n: sample size per variant
description: {"references": ["De Angelis F, Zeleznik OA, Wendt FR, Pathak GA, Tylee DS, De Lillo A, Koller D, Cabrera-Mendoza B, Clifford RE, Maihofer AX, Nievergelt CM, Curhan GC, Curhan SG, Polimanti R. Sex differences in the polygenic architecture of hearing problems in adults. Genome Med. https://doi.org/10.1186/s13073-023-01186-3"]}
DOI: 10.5281/zenodo.7897037
title: Genome-wide association statistics of Hearing Problems

description: Genome-wide Association Statistics of Hearing Problems Citation: De Angelis F, Zeleznik OA, Wendt FR, Pathak GA, Tylee DS, De Lillo A, Koller D, Cabrera-Mendoza B, Clifford RE, Maihofer AX, Nievergelt CM, Curhan GC, Curhan SG, Polimanti R. Sex differences in the polygenic architecture of hearing problems in adults. Genome Med. https://doi.org/10.1186/s13073-023-01186-3 COLUMN HEADERS<br> chromosome: chromosome<br> base_pair_location: position<br> effect_allele: effect allele (corresponds to the effect size’s sign; may not be the alternate allele)<br> other_allele: non-effect allele<br> beta: effect measured as beta, sign corresponds to the effect of the effect allele<br> standard_error: standard error of the effect<br> effect_allele_frequency: effect allele frequency in UK Biobank participants of European descent<br> p_value: p value of the association statistic<br> variant_id: variant identifier<br> rs_id: rsID of the variant<br> n: sample size per variant
description: {"references": ["De Angelis F, Zeleznik OA, Wendt FR, Pathak GA, Tylee DS, De Lillo A, Koller D, Cabrera-Mendoza B, Clifford RE, Maihofer AX, Nievergelt CM, Curhan GC, Curhan SG, Polimanti R. Sex differences in the polygenic architecture of hearing problems in adults. Genome Med. https://doi.org/10.1186/s13073-023-01186-3"]}
DOI: 10.25345/c5g737d8j
title: MassIVE MSV000091857 - Nanodisc Assembly E. coli and Brain Lipids
title: Data set for lipidomic analysis of nanodiscs assembled with different temperatures, belt sizes, and lipid types, including both E. coli and porcine brain polar lipid extracts.
DOI: 10.5517/ccdc.csd.cc28ytln
title: CCDC 2114032: Experimental Crystal Structure Determination

description: Related Article: Georg Niggemeyer, Anastasia Knyazeva, Raphael Gasper, Dale Corkery, Pia Bodenbinder, Julian J. Holstein, Sonja Sievers, Yao-Wen Wu, Herbert Waldmann|2022|Angew.Chem.,Int.Ed.|61|e202114328|doi:10.1002/anie.202114328
description: An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.
DOI: 10.5281/zenodo.7427640
title: Computer-rendered HDR and LDR 4k images database

description: Realistic image computation mimics the natural process of acquiring pictures by simulating the physical interactions of light between all the objects, lights and cameras lying within a modelled 3D scene. This process is known as global illumination and was formalised by Kajiya with the following rendering Equation:<br> \(\begin{equation} \label{eq:rendering_equation} L_o(x, \omega_o) = {L_e(x, \omega_o)} + \int_{\Omega}^{} {L_i(x, \omega_i)} \cdot f_r(x, \omega_i \rightarrow \omega_o) \cdot \cos \theta_i d\omega_i \end{equation}\) where: \(L_o(x, \omega_o)\) is the luminance traveling from point \(x\) in direction \(\omega_o\); \(L_e(x, \omega_o)\) is point \(x\) emitted luminance (it is null if point x does not lie on a ligth source surface); the integral represents the set of luminances \(L_i\)incident in \(x \) from the hemisphere of the directions \(\Omega\) and reflected in the direction \(\omega_o\). The reflected luminances are weighted by the materials reflecting properties (bidirectionnal reflectance function \(f_r(x, \omega_i \rightarrow \omega_o)\)) and the cosinus of the incident angle. This equation cannot be analytically solved and Monte Carlo approaches are generally used to estimate the value of the pixels of the final image. This proposed dataset is composed of 32 points of view of photo realistics images with different level of samples (following the Monte Carlo approach) for each. Each image is 3840 × 2160 pixels in size. The most noisy image is of 2⁰ samples and the reference one (the most converged image obtained) is of 2²⁰ samples. The pbrt rendering engine (version 4) was used to generate these images.
DOI: 10.5281/zenodo.7427639
title: Computer-rendered HDR and LDR 4k images database

description: Realistic image computation mimics the natural process of acquiring pictures by simulating the physical interactions of light between all the objects, lights and cameras lying within a modelled 3D scene. This process is known as global illumination and was formalised by Kajiya with the following rendering Equation:<br> \(\begin{equation} \label{eq:rendering_equation} L_o(x, \omega_o) = {L_e(x, \omega_o)} + \int_{\Omega}^{} {L_i(x, \omega_i)} \cdot f_r(x, \omega_i \rightarrow \omega_o) \cdot \cos \theta_i d\omega_i \end{equation}\) where: \(L_o(x, \omega_o)\) is the luminance traveling from point \(x\) in direction \(\omega_o\); \(L_e(x, \omega_o)\) is point \(x\) emitted luminance (it is null if point x does not lie on a ligth source surface); the integral represents the set of luminances \(L_i\)incident in \(x \) from the hemisphere of the directions \(\Omega\) and reflected in the direction \(\omega_o\). The reflected luminances are weighted by the materials reflecting properties (bidirectionnal reflectance function \(f_r(x, \omega_i \rightarrow \omega_o)\)) and the cosinus of the incident angle. This equation cannot be analytically solved and Monte Carlo approaches are generally used to estimate the value of the pixels of the final image. This proposed dataset is composed of 32 points of view of photo realistics images with different level of samples (following the Monte Carlo approach) for each. Each image is 3840 × 2160 pixels in size. The most noisy image is of 2⁰ samples and the reference one (the most converged image obtained) is of 2²⁰ samples. The pbrt rendering engine (version 4) was used to generate these images.
DOI: 10.6084/m9.figshare.22762466
title: Demographic Diagnostic and ALR transformed microbiome data

description: The alr file also contains for: Factor scores for 3 person-wise factors of butyrate-producers (btf1, btf2 and btf3) Factor scores for 3 person-wise factors of probiotic taxa (pbf1, pbf2, pbf3) The cluster designation from the staggered interaction random forest (sid1c) The person-wise distances from the staggered interaction random forest (sid1d) The person-wise ordinates from the KODAMA analysis (k11 and k12) The person-wise dissimilarity scores from the KODAMA analysis (k1dis) The person-wise proximity scores from the KODAMA analysis (k1prox) The person-wise ‘costs’ from the KODAMA analysis
DOI: 10.6084/m9.figshare.22762466.v1
title: Demographic Diagnostic and ALR transformed microbiome data

description: The alr file also contains for: Factor scores for 3 person-wise factors of butyrate-producers (btf1, btf2 and btf3) Factor scores for 3 person-wise factors of probiotic taxa (pbf1, pbf2, pbf3) The cluster designation from the staggered interaction random forest (sid1c) The person-wise distances from the staggered interaction random forest (sid1d) The person-wise ordinates from the KODAMA analysis (k11 and k12) The person-wise dissimilarity scores from the KODAMA analysis (k1dis) The person-wise proximity scores from the KODAMA analysis (k1prox) The person-wise ‘costs’ from the KODAMA analysis
DOI: 10.35078/jkklhm
title: Replication Data for: Ficha epidemiológica de localidade: Distrito: Diamantina | Município: Curvelo

description: Levantamento Triatomínico com operações de campo ocorridas em Minas Gerais pela Superintendência de Campanhas de Saúde Pública (SUCAM) e FUNASA (Fundação Nacional de Saúde), no período de 1979 a 1999, objetivando a busca da presença de vetores da doença de Chagas ou de vestígios dessa presença. A partir dela são orientadas as operações com inseticida (pt) Triatomine survey with field operations carried out in Minas Gerais by the Public Health Campaigns Superintendence (SUCAM) and FUNASA (National Health Foundation), from 1979 to 1999, aiming to search for the presence of Chagas disease vectors or traces of that presence. From it, operations with insecticide are guided (en) Encuesta de triatominos con operaciones de campo realizada en Minas Gerais por la Superintendencia de Campañas de Salud Pública (SUCAM) y FUNASA (Fundación Nacional de Salud), de 1979 a 1999, con el objetivo de buscar la presencia de vectores de la enfermedad de Chagas o rastros de esa presencia. Desde ella se orientan las operaciones con insecticida (es)
DOI: 10.17188/1753296
title: Materials Data on Al2Fe2Bi2O9 by Materials Project

description: Fe2Al2Bi2O9 crystallizes in the orthorhombic Pbam space group. The structure is three-dimensional. Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with four equivalent AlO6 octahedra and a cornercorner with one FeO4 tetrahedra. The corner-sharing octahedra tilt angles range from 50–58°. There are a spread of Fe–O bond distances ranging from 1.86–1.92 Å. Al3+ is bonded to six O2- atoms to form AlO6 octahedra that share corners with four equivalent FeO4 tetrahedra and edges with two equivalent AlO6 octahedra. There are a spread of Al–O bond distances ranging from 1.90–1.98 Å. Bi3+ is bonded in a 4-coordinate geometry to six O2- atoms. There are a spread of Bi–O bond distances ranging from 2.15–3.02 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal planar geometry to one Fe3+, one Al3+, and two equivalent Bi3+ atoms. In the second O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Al3+ and two equivalent Bi3+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Fe3+ and two equivalent Al3+ atoms. In the fourth O2- site, O2- is bonded in a linear geometry to two equivalent Fe3+ atoms.
DOI: 10.17188/1753297
title: Materials Data on TbCdPd by Materials Project

description: TbPdCd crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Tb is bonded in a 11-coordinate geometry to five Pd and six equivalent Cd atoms. There are four shorter (3.04 Å) and one longer (3.12 Å) Tb–Pd bond lengths. There are two shorter (3.24 Å) and four longer (3.36 Å) Tb–Cd bond lengths. There are two inequivalent Pd sites. In the first Pd site, Pd is bonded in a 9-coordinate geometry to three equivalent Tb and six equivalent Cd atoms. All Pd–Cd bond lengths are 2.78 Å. In the second Pd site, Pd is bonded in a 9-coordinate geometry to six equivalent Tb and three equivalent Cd atoms. All Pd–Cd bond lengths are 2.89 Å. Cd is bonded in a 10-coordinate geometry to six equivalent Tb and four Pd atoms.
DOI: 10.17188/1753298
title: Materials Data on Fe10O11F9 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: 10.17188/1753299
title: Materials Data on SnTe2Pb by Materials Project

description: PbSnTe2 is Caswellsilverite-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. Pb2+ is bonded to six Te2- atoms to form PbTe6 octahedra that share corners with six equivalent PbTe6 octahedra, edges with four equivalent PbTe6 octahedra, and edges with eight equivalent SnTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (3.24 Å) and two longer (3.25 Å) Pb–Te bond lengths. Sn2+ is bonded to six Te2- atoms to form SnTe6 octahedra that share corners with six equivalent SnTe6 octahedra, edges with four equivalent SnTe6 octahedra, and edges with eight equivalent PbTe6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are four shorter (3.24 Å) and two longer (3.25 Å) Sn–Te bond lengths. There are two inequivalent Te2- sites. In the first Te2- site, Te2- is bonded to two equivalent Pb2+ and four equivalent Sn2+ atoms to form a mixture of corner and edge-sharing TeSn4Pb2 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second Te2- site, Te2- is bonded to four equivalent Pb2+ and two equivalent Sn2+ atoms to form TeSn2Pb4 octahedra that share corners with six equivalent TeSn2Pb4 octahedra and edges with twelve TeSn4Pb2 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1753300
title: Materials Data on SrScO3 by Materials Project

description: SrScO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Sr is bonded to twelve equivalent O atoms to form SrO12 cuboctahedra that share corners with twelve equivalent SrO12 cuboctahedra, faces with six equivalent SrO12 cuboctahedra, and faces with eight equivalent ScO6 octahedra. All Sr–O bond lengths are 2.93 Å. Sc is bonded to six equivalent O atoms to form ScO6 octahedra that share corners with six equivalent ScO6 octahedra and faces with eight equivalent SrO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Sc–O bond lengths are 2.07 Å. O is bonded in a distorted linear geometry to four equivalent Sr and two equivalent Sc atoms.
DOI: 10.17188/1753301
title: Materials Data on Lu4Ni by Materials Project

description: Lu4Ni is Iron carbide-like structured and crystallizes in the cubic Fd-3m space group. The structure is zero-dimensional and consists of eight Lu4Ni clusters. Lu is bonded in a single-bond geometry to one Ni atom. The Lu–Ni bond length is 2.48 Å. Ni is bonded in a tetrahedral geometry to four equivalent Lu atoms.
DOI: 10.17188/1753302
title: Materials Data on KBiS2 by Materials Project

description: KBiS2 is Caswellsilverite-like structured and crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. K1+ is bonded to six S2- atoms to form KS6 octahedra that share corners with six equivalent KS6 octahedra, edges with four equivalent KS6 octahedra, and edges with eight equivalent BiS6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.90 Å) and four longer (3.01 Å) K–S bond lengths. Bi3+ is bonded to six S2- atoms to form BiS6 octahedra that share corners with six equivalent BiS6 octahedra, edges with four equivalent BiS6 octahedra, and edges with eight equivalent KS6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are two shorter (2.90 Å) and four longer (3.01 Å) Bi–S bond lengths. There are two inequivalent S2- sites. In the first S2- site, S2- is bonded to two equivalent K1+ and four equivalent Bi3+ atoms to form a mixture of edge and corner-sharing SK2Bi4 octahedra. The corner-sharing octahedral tilt angles are 0°. In the second S2- site, S2- is bonded to four equivalent K1+ and two equivalent Bi3+ atoms to form SK4Bi2 octahedra that share corners with six equivalent SK4Bi2 octahedra and edges with twelve SK2Bi4 octahedra. The corner-sharing octahedral tilt angles are 0°.
DOI: 10.17188/1753303
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: 10.17188/1753304
title: Materials Data on HgWO4 by Materials Project

description: HgWO4 crystallizes in the orthorhombic Cmce space group. The structure is three-dimensional. W6+ is bonded to six O2- atoms to form a mixture of distorted edge and corner-sharing WO6 pentagonal pyramids. There are a spread of W–O bond distances ranging from 1.81–2.07 Å. Hg2+ is bonded in a 2-coordinate geometry to seven O2- atoms. There are a spread of Hg–O bond distances ranging from 2.19–2.81 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent W6+ and three equivalent Hg2+ atoms. In the second O2- site, O2- is bonded in a trigonal non-coplanar geometry to one W6+ and two equivalent Hg2+ atoms. In the third O2- site, O2- is bonded in a water-like geometry to two equivalent W6+ atoms. In the fourth O2- site, O2- is bonded in a distorted single-bond geometry to one W6+ and two equivalent Hg2+ atoms.
DOI: 10.17188/1753305
title: Materials Data on MgSi2 by Materials Project

description: MgSi2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Mg sites. In the first Mg site, Mg is bonded in a 12-coordinate geometry to two equivalent Mg and ten Si atoms. There are one shorter (3.08 Å) and one longer (3.15 Å) Mg–Mg bond lengths. There are a spread of Mg–Si bond distances ranging from 2.77–3.20 Å. In the second Mg site, Mg is bonded in a 2-coordinate geometry to two equivalent Mg and seven Si atoms. There are a spread of Mg–Si bond distances ranging from 2.65–3.08 Å. In the third Mg site, Mg is bonded in a 5-coordinate geometry to six Si atoms. There are a spread of Mg–Si bond distances ranging from 2.72–3.17 Å. In the fourth Mg site, Mg is bonded in a 7-coordinate geometry to ten Si atoms. There are a spread of Mg–Si bond distances ranging from 2.80–3.17 Å. There are eight inequivalent Si sites. In the first Si site, Si is bonded in a 1-coordinate geometry to four Mg and three Si atoms. There are two shorter (2.38 Å) and one longer (2.50 Å) Si–Si bond lengths. 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 2.43–2.93 Å. In the third Si site, Si is bonded in a 4-coordinate geometry to five Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.48–2.78 Å. In the fourth Si site, Si is bonded in a 6-coordinate geometry to four Mg and three Si atoms. There are a spread of Si–Si bond distances ranging from 2.40–2.50 Å. In the fifth Si site, Si is bonded in a 8-coordinate geometry to five Mg and three Si atoms. In the sixth Si site, Si is bonded in a 7-coordinate geometry to three Mg and four Si atoms. In the seventh Si site, Si is bonded in a 6-coordinate geometry to three Mg and three Si atoms. In the eighth Si site, Si is bonded in a 1-coordinate geometry to four Mg and four Si atoms.
DOI: 10.17188/1753306
title: Materials Data on YbCeMg2 by Materials Project

description: Mg2YbCe is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to four equivalent Yb and four equivalent Ce atoms. All Mg–Yb bond lengths are 3.37 Å. All Mg–Ce bond lengths are 3.37 Å. Yb is bonded in a body-centered cubic geometry to eight equivalent Mg atoms. Ce is bonded in a body-centered cubic geometry to eight equivalent Mg atoms.
DOI: 10.17188/1753308
title: Materials Data on LiCoPO4 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: 10.17188/1753309
title: Materials Data on RbCrH24(SO10)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: 10.17188/1753311
title: Materials Data on Y3Ga by Materials Project

description: Y3Ga is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Y is bonded to eight equivalent Y and four equivalent Ga atoms to form distorted YY8Ga4 cuboctahedra that share corners with twelve equivalent YY8Ga4 cuboctahedra, edges with eight equivalent GaY12 cuboctahedra, edges with sixteen equivalent YY8Ga4 cuboctahedra, faces with four equivalent GaY12 cuboctahedra, and faces with fourteen equivalent YY8Ga4 cuboctahedra. All Y–Y bond lengths are 3.36 Å. All Y–Ga bond lengths are 3.36 Å. Ga is bonded to twelve equivalent Y atoms to form GaY12 cuboctahedra that share corners with twelve equivalent GaY12 cuboctahedra, edges with twenty-four equivalent YY8Ga4 cuboctahedra, faces with six equivalent GaY12 cuboctahedra, and faces with twelve equivalent YY8Ga4 cuboctahedra.