cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17188/1313964
title: Materials Data on La3Dy by Materials Project

description: DyLa3 is beta Cu3Ti-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Dy is bonded to twelve La atoms to form DyLa12 cuboctahedra that share corners with four equivalent DyLa12 cuboctahedra, corners with eight equivalent LaLa8Dy4 cuboctahedra, edges with eight equivalent DyLa12 cuboctahedra, edges with sixteen equivalent LaLa8Dy4 cuboctahedra, faces with four equivalent DyLa12 cuboctahedra, and faces with fourteen LaLa8Dy4 cuboctahedra. There are four shorter (3.68 Å) and eight longer (3.69 Å) Dy–La bond lengths. There are two inequivalent La sites. In the first La site, La is bonded to four equivalent Dy and eight La atoms to form LaLa8Dy4 cuboctahedra that share corners with twelve equivalent LaLa8Dy4 cuboctahedra, edges with eight equivalent DyLa12 cuboctahedra, edges with sixteen LaLa8Dy4 cuboctahedra, faces with four equivalent DyLa12 cuboctahedra, and faces with fourteen LaLa8Dy4 cuboctahedra. There are four shorter (3.68 Å) and four longer (3.69 Å) La–La bond lengths. In the second La site, La is bonded to four equivalent Dy and eight equivalent La atoms to form LaLa8Dy4 cuboctahedra that share corners with four equivalent LaLa8Dy4 cuboctahedra, corners with eight equivalent DyLa12 cuboctahedra, edges with twenty-four LaLa8Dy4 cuboctahedra, faces with six equivalent DyLa12 cuboctahedra, and faces with twelve LaLa8Dy4 cuboctahedra.
DOI: 10.17188/1313965
title: Materials Data on La3Er by Materials Project

description: ErLa3 is beta Cu3Ti-like structured and crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Er is bonded to twelve La atoms to form ErLa12 cuboctahedra that share corners with four equivalent ErLa12 cuboctahedra, corners with eight equivalent LaLa8Er4 cuboctahedra, edges with eight equivalent ErLa12 cuboctahedra, edges with sixteen equivalent LaLa8Er4 cuboctahedra, faces with four equivalent ErLa12 cuboctahedra, and faces with fourteen LaLa8Er4 cuboctahedra. There are four shorter (3.68 Å) and eight longer (3.69 Å) Er–La bond lengths. There are two inequivalent La sites. In the first La site, La is bonded to four equivalent Er and eight La atoms to form LaLa8Er4 cuboctahedra that share corners with twelve equivalent LaLa8Er4 cuboctahedra, edges with eight equivalent ErLa12 cuboctahedra, edges with sixteen LaLa8Er4 cuboctahedra, faces with four equivalent ErLa12 cuboctahedra, and faces with fourteen LaLa8Er4 cuboctahedra. There are four shorter (3.68 Å) and four longer (3.69 Å) La–La bond lengths. In the second La site, La is bonded to four equivalent Er and eight equivalent La atoms to form LaLa8Er4 cuboctahedra that share corners with four equivalent LaLa8Er4 cuboctahedra, corners with eight equivalent ErLa12 cuboctahedra, edges with twenty-four LaLa8Er4 cuboctahedra, faces with six equivalent ErLa12 cuboctahedra, and faces with twelve LaLa8Er4 cuboctahedra.
DOI: 10.17188/1313966
title: Materials Data on Sc2AlCd by Materials Project

description: Sc2CdAl 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 Cd and four equivalent Al atoms. All Sc–Cd bond lengths are 3.01 Å. All Sc–Al bond lengths are 3.01 Å. Cd is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Al is bonded in a body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1313967
title: Materials Data on MgCu by Materials Project

description: MgCu is Tetraauricupride structured and crystallizes in the orthorhombic Pmma space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Cu atoms. There are a spread of Mg–Cu bond distances ranging from 2.69–2.77 Å. Cu is bonded in a body-centered cubic geometry to eight equivalent Mg atoms.
DOI: 10.17188/1313968
title: Materials Data on La(Mg4Al3)4 by Materials Project

description: La(Mg4Al3)4 crystallizes in the cubic I-43m space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded in a 12-coordinate geometry to seven Mg and five equivalent Al atoms. There are a spread of Mg–Mg bond distances ranging from 3.01–3.18 Å. There are a spread of Mg–Al bond distances ranging from 2.84–3.17 Å. In the second Mg site, Mg is bonded in a 10-coordinate geometry to three equivalent Mg, one La, and six equivalent Al atoms. The Mg–La bond length is 3.34 Å. All Mg–Al bond lengths are 3.23 Å. La is bonded in a 12-coordinate geometry to four equivalent Mg and twelve equivalent Al atoms. All La–Al bond lengths are 3.27 Å. Al is bonded in a 11-coordinate geometry to seven Mg, one La, and three equivalent Al atoms. There are one shorter (2.75 Å) and two longer (2.81 Å) Al–Al bond lengths.
DOI: 10.17188/1313969
title: Materials Data on ScZn2Au by Materials Project

description: ScAuZn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sc is bonded in a 8-coordinate geometry to six equivalent Au and eight equivalent Zn atoms. All Sc–Au bond lengths are 3.22 Å. All Sc–Zn bond lengths are 2.79 Å. Au is bonded in a distorted body-centered cubic geometry to six equivalent Sc and eight equivalent Zn atoms. All Au–Zn bond lengths are 2.79 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Sc and four equivalent Au atoms.
DOI: 10.17188/1313970
title: Materials Data on EuMgO3 by Materials Project

description: MgEuO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Mg is bonded to six equivalent O atoms to form MgO6 octahedra that share corners with six equivalent MgO6 octahedra and faces with eight equivalent EuO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Mg–O bond lengths are 1.96 Å. Eu is bonded to twelve equivalent O atoms to form EuO12 cuboctahedra that share corners with twelve equivalent EuO12 cuboctahedra, faces with six equivalent EuO12 cuboctahedra, and faces with eight equivalent MgO6 octahedra. All Eu–O bond lengths are 2.77 Å. O is bonded in a distorted linear geometry to two equivalent Mg and four equivalent Eu atoms.
DOI: 10.17188/1313971
title: Materials Data on ScZnNi2 by Materials Project

description: ScNi2Zn 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 eight equivalent Ni atoms. All Sc–Ni bond lengths are 2.62 Å. Ni is bonded in a body-centered cubic geometry to four equivalent Sc and four equivalent Zn atoms. All Ni–Zn bond lengths are 2.62 Å. Zn is bonded in a distorted body-centered cubic geometry to eight equivalent Ni atoms.
DOI: 10.17188/1313972
title: Materials Data on ScAlCO by Materials Project

description: ScAlOC crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are two inequivalent Sc3+ sites. In the first Sc3+ site, Sc3+ is bonded to six equivalent C4- atoms to form ScC6 octahedra that share corners with six equivalent AlC3O tetrahedra, edges with six equivalent ScC6 octahedra, and edges with six equivalent AlC3O tetrahedra. All Sc–C bond lengths are 2.40 Å. In the second Sc3+ site, Sc3+ is bonded to six equivalent O2- atoms to form ScO6 octahedra that share corners with six equivalent AlC3O tetrahedra and edges with six equivalent ScO6 octahedra. All Sc–O bond lengths are 2.15 Å. Al3+ is bonded to three equivalent C4- and one O2- atom to form AlC3O tetrahedra that share corners with six ScC6 octahedra, corners with six equivalent AlC3O tetrahedra, and edges with three equivalent ScC6 octahedra. The corner-sharing octahedra tilt angles range from 17–62°. All Al–C bond lengths are 2.03 Å. The Al–O bond length is 1.86 Å. C4- is bonded to three equivalent Sc3+ and three equivalent Al3+ atoms to form distorted CSc3Al3 octahedra that share corners with three equivalent CSc3Al3 octahedra, corners with three equivalent OSc3Al tetrahedra, and edges with nine equivalent CSc3Al3 octahedra. The corner-sharing octahedral tilt angles are 0°. O2- is bonded to three equivalent Sc3+ and one Al3+ atom to form distorted OSc3Al tetrahedra that share corners with three equivalent CSc3Al3 octahedra, corners with nine equivalent OSc3Al tetrahedra, and edges with three equivalent OSc3Al tetrahedra. The corner-sharing octahedral tilt angles are 69°.
DOI: 10.17188/1313973
title: Materials Data on NaBi3 by Materials Project

description: NaBi3 is Uranium Silicide-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Na is bonded to twelve equivalent Bi atoms to form a mixture of corner and face-sharing NaBi12 cuboctahedra. There are six shorter (3.51 Å) and six longer (3.52 Å) Na–Bi bond lengths. Bi is bonded in a distorted see-saw-like geometry to four equivalent Na atoms.
DOI: 10.17188/1313974
title: Materials Data on HoErAg2 by Materials Project

description: ErHoAg2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Er–Ag bond lengths are 3.13 Å. Ho is bonded in a body-centered cubic geometry to eight equivalent Ag atoms. All Ho–Ag bond lengths are 3.13 Å. Ag is bonded in a body-centered cubic geometry to four equivalent Er and four equivalent Ho atoms.
DOI: 10.17188/1313975
title: Materials Data on LaSmZn2 by Materials Project

description: SmLaZn2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sm is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All Sm–Zn bond lengths are 3.21 Å. La is bonded in a body-centered cubic geometry to eight equivalent Zn atoms. All La–Zn bond lengths are 3.21 Å. Zn is bonded in a body-centered cubic geometry to four equivalent Sm and four equivalent La atoms.
DOI: 10.17188/1313976
title: Materials Data on MgCd2 by Materials Project

description: MgCd2 crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Mg is bonded to three equivalent Mg and nine Cd atoms to form MgMg3Cd9 cuboctahedra that share corners with nine equivalent MgMg3Cd9 cuboctahedra, corners with nine equivalent CdMg6Cd6 cuboctahedra, edges with six equivalent MgMg3Cd9 cuboctahedra, edges with twelve equivalent CdMg4Cd8 cuboctahedra, faces with five equivalent MgMg3Cd9 cuboctahedra, and faces with fifteen CdMg4Cd8 cuboctahedra. All Mg–Mg bond lengths are 3.14 Å. There are three shorter (3.14 Å) and six longer (3.16 Å) Mg–Cd bond lengths. There are two inequivalent Cd sites. In the first Cd site, Cd is bonded to four equivalent Mg and eight Cd atoms to form CdMg4Cd8 cuboctahedra that share corners with eighteen equivalent CdMg4Cd8 cuboctahedra, edges with eight equivalent MgMg3Cd9 cuboctahedra, edges with ten CdMg4Cd8 cuboctahedra, faces with eight equivalent MgMg3Cd9 cuboctahedra, and faces with twelve CdMg4Cd8 cuboctahedra. There are a spread of Cd–Cd bond distances ranging from 3.13–3.16 Å. In the second Cd site, Cd is bonded to six equivalent Mg and six equivalent Cd atoms to form distorted CdMg6Cd6 cuboctahedra that share corners with eighteen equivalent MgMg3Cd9 cuboctahedra, edges with eighteen CdMg4Cd8 cuboctahedra, faces with six equivalent MgMg3Cd9 cuboctahedra, and faces with fourteen CdMg4Cd8 cuboctahedra.
DOI: 10.17188/1313977
title: Materials Data on ScTiRu2 by Materials Project

description: ScTiRu2 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 eight equivalent Ru atoms. All Sc–Ru bond lengths are 2.72 Å. Ti is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ti–Ru bond lengths are 2.72 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Sc and four equivalent Ti atoms.
DOI: 10.17188/1313978
title: Materials Data on La2IrAu by Materials Project

description: La2IrAu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. La is bonded in a body-centered cubic geometry to four equivalent Ir and four equivalent Au atoms. All La–Ir bond lengths are 3.19 Å. All La–Au bond lengths are 3.19 Å. Ir is bonded in a body-centered cubic geometry to eight equivalent La atoms. Au is bonded in a body-centered cubic geometry to eight equivalent La atoms.
DOI: 10.17188/1313979
title: Materials Data on Sc2NiRh by Materials Project

description: Sc2RhNi 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 Rh and four equivalent Ni atoms. All Sc–Rh bond lengths are 2.78 Å. All Sc–Ni bond lengths are 2.78 Å. Rh is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Ni is bonded in a body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1313980
title: Materials Data on GdF3 by Materials Project

description: GdF3 is alpha bismuth trifluoride structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Gd3+ is bonded in a distorted body-centered cubic geometry to fourteen F1- atoms. There are eight shorter (2.45 Å) and six longer (2.83 Å) Gd–F bond lengths. There are two inequivalent F1- sites. In the first F1- site, F1- is bonded to four equivalent Gd3+ and four equivalent F1- atoms to form a mixture of corner, edge, and face-sharing FGd4F4 tetrahedra. All F–F bond lengths are 2.45 Å. In the second F1- site, F1- is bonded in a 6-coordinate geometry to six equivalent Gd3+ and eight equivalent F1- atoms.
DOI: 10.17188/1313981
title: Materials Data on Sc2OsAu by Materials Project

description: Sc2OsAu 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 Au atoms. All Sc–Os bond lengths are 2.86 Å. All Sc–Au bond lengths are 2.86 Å. Os is bonded in a body-centered cubic geometry to eight equivalent Sc atoms. Au is bonded in a body-centered cubic geometry to eight equivalent Sc atoms.
DOI: 10.17188/1313982
title: Materials Data on ScSiRh2 by Materials Project

description: ScRh2Si 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 eight equivalent Rh atoms. All Sc–Rh bond lengths are 2.67 Å. Rh is bonded in a body-centered cubic geometry to four equivalent Sc and four equivalent Si atoms. All Rh–Si bond lengths are 2.67 Å. Si is bonded in a distorted body-centered cubic geometry to eight equivalent Rh atoms.
DOI: 10.5281/zenodo.7704359
title: Measurements of rate coefficients of CN+, HCN+ and HNC+ collisions with H2 at cryogenic temperatures

description: Raw experimental data and post-processing scripts for DOI: 10.1063/5.0153699
DOI: 10.5281/zenodo.7704358
title: Measurements of rate coefficients of CN+, HCN+ and HNC+ collisions with H2 at cryogenic temperatures

description: Raw experimental data and post-processing scripts for DOI: 10.1063/5.0153699
DOI: 10.5281/zenodo.8006845
title: Data generated for 'Early stage of Erythrocyte Sedimentation Rate test: Fracture of a high-volume-fraction gel'

description: This dataset has been generated for the manuscript entitled "Early stage of Erythrocyte Sedimentation Rate test: Fracture of a high-volume-fraction gel".
DOI: 10.5281/zenodo.8006846
title: Data generated for 'Early stage of Erythrocyte Sedimentation Rate test: Fracture of a high-volume-fraction gel'

description: This dataset has been generated for the manuscript entitled "Early stage of Erythrocyte Sedimentation Rate test: Fracture of a high-volume-fraction gel".
DOI: 10.34740/kaggle/dsv/5854703
title: AutoXGB
DOI: 10.5281/zenodo.7794565
title: Automated mapping and classification of valleys beneath the Greenland Ice Sheet: Datasets

description: <strong>Valley morphology and classification: training dataset and full dataset for Greenland</strong> This dataset contains: TrainingDataValleys.csv: A .csv file of the training dataset used to classify valleys in Greenland as 'fluvial' or 'glacial'. These valleys were extracted from the Copernicus 90 m global digital elevation model. GreenlandValleys.csv: A .csv file of the locations, morphometrics, and class of Greenland valleys identified in Operation IceBridge and CReSIS radio-echo sounding data. These valleys have been classified using a random forest model trained using the above training dataset.
DOI: 10.5281/zenodo.7794564
title: Automated mapping and classification of valleys beneath the Greenland Ice Sheet: Datasets

description: <strong>Valley morphology and classification: training dataset and full dataset for Greenland</strong> This dataset contains: TrainingDataValleys.csv: A .csv file of the training dataset used to classify valleys in Greenland as 'fluvial' or 'glacial'. These valleys were extracted from the Copernicus 90 m global digital elevation model. GreenlandValleys.csv: A .csv file of the locations, morphometrics, and class of Greenland valleys identified in Operation IceBridge and CReSIS radio-echo sounding data. These valleys have been classified using a random forest model trained using the above training dataset.
DOI: 10.5281/zenodo.7892452
title: 3D ToF MPI multi-frequency mesh dataset

description: The accuracy of indirect 3D Time-of-Flight (3D ToF) measurements is often limited by multi-path interferences (MPI) caused by multi-layer ToF conditions. Taking multiple measurements of the same scene at different modulation frequencies allows separating the interfering signal components of the individual paths according to several optimization methods described in literature. Orthogonal matching pursuit (OMP) optimization has been reported to achieve good path separation performance and superior results compared to particle swarm optimization (PSO). This work presents improved PSO performance for MPI separation based on new experimental data and refined PSO strategy. The current PSO approach achieves good distance separation in the setup used with low RMS distance errors in the order of 20 cm in situations where the OMP approach shows RMS errors higher than 100 cm. The previously reported minimum distance difference limitation between two separate objects of 2.7 m for the OMP algorithm could be reduced to roughly 0.75 m for the PSO algorithm. The trade-off between image accuracy and computing effort is explored and presented with respect to PSO parameter settings. This dataset provides researchers with measurement data to develop their own multi-layer algorithms and contribute to the ongoing development of great 3D ToF cameras.
DOI: 10.5281/zenodo.7892451
title: 3D ToF MPI multi-frequency mesh dataset

description: The accuracy of indirect 3D Time-of-Flight (3D ToF) measurements is often limited by multi-path interferences (MPI) caused by multi-layer ToF conditions. Taking multiple measurements of the same scene at different modulation frequencies allows separating the interfering signal components of the individual paths according to several optimization methods described in literature. Orthogonal matching pursuit (OMP) optimization has been reported to achieve good path separation performance and superior results compared to particle swarm optimization (PSO). This work presents improved PSO performance for MPI separation based on new experimental data and refined PSO strategy. The current PSO approach achieves good distance separation in the setup used with low RMS distance errors in the order of 20 cm in situations where the OMP approach shows RMS errors higher than 100 cm. The previously reported minimum distance difference limitation between two separate objects of 2.7 m for the OMP algorithm could be reduced to roughly 0.75 m for the PSO algorithm. The trade-off between image accuracy and computing effort is explored and presented with respect to PSO parameter settings. This dataset provides researchers with measurement data to develop their own multi-layer algorithms and contribute to the ongoing development of great 3D ToF cameras.
DOI: 10.1594/wdcc/hoaps2_monthly
title: Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data - HOAPS II - monthly mean

description: Project: Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data - For more information see http://www.hoaps.zmaw.de/ Summary: The new version of the Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data set - HOAPS II - contains improved global fields of precipitation and evaporation over the oceans and all basic state variables needed for the derivation of the turbulent fluxes. Except for the NOAA Pathfinder SST data set, all variables are derived from SSM/I satellite data over the ice free oceans between 1987 and 2002. The earlier HOAPS version was improved and includes now the utilisation of multi-satellite averages with proper inter-satellite calibration, improved algorithms and a new ice detection procedure, resulting in more homogeneous and reliable spatial and temporal fields as before. The spatial resolution of 0.5 degree, makes them ideally suited for studies of climate variability over the global oceans. Pentade and climatological means are also public and available via the CERA database system. Further information under : http://www.hoaps.zmaw.de .
DOI: 10.1594/wdcc/hoaps2_pentad
title: Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data - HOAPS II - 5-days mean

description: Project: Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data - For more information see http://www.hoaps.zmaw.de/ Summary: The new version of the Hamburg Ocean Atmosphere Parameters and Fluxes from Satellite Data set - HOAPS II - contains improved global fields of precipitation and evaporation over the oceans and all basic state variables needed for the derivation of the turbulent fluxes. Except for the NOAA Pathfinder SST data set, all variables are derived from SSM/I satellite data over the ice free oceans between 1987 and 2002. The earlier HOAPS version was improved and includes now the utilisation of multi-satellite averages with proper inter-satellite calibration, improved algorithms and a new ice detection procedure, resulting in more homogeneous and reliable spatial and temporal fields as before. Here, 5-days mean( Pentad )datasets are available but monthly mean and climatological means are also public and available via the CERA database system. The spatial resolution of 0.5 degree, makes them ideally suited for studies of climate variability over the global oceans. Further information under : http://www.hoaps.zmaw.de .
DOI: 10.5281/zenodo.7971738
title: CESM1.2 simulation data for "CO2 and orbitally driven oxygen isotope variability in the Early Eocene"

description: CESM1.2 simulation data for the Early Eocene. These are atmosphere and land climatology files for simulations at both 3x and 6x pre-industrial CO2 levels, as well as 4 separate orbits. The climatology was averaged over the last 100 years of each simulation.
DOI: 10.5281/zenodo.7986868
title: IsoCloud4 Data Sets for Depositional Ice Growth Analysis

description: Data sets used in the publication <strong>Re-evaluating cloud chamber constraints on depositional ice growth in cirrus clouds--<br> Part 1: Model description and sensitivity tests </strong><br> K.D. Lamb, J. Harrington, B.W. Clouser, E.J. Moyer, L. Sarkozy, V. Ebert, O. Möhler, H. Saathoff.<br> <em>Atmospheric Chemistry and Physics </em>(2023)