cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.70879.v1/t63
title: "Table 63" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Statistical covariance matrix for the $6\times3$ bins of the normalized differential cross section as a function of $\cos\theta^{\star}_{\ell^+} \cos\theta^{\star}_{\ell^-}$ and $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t64
title: "Table 64" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Systematic covariance matrix for the $6\times3$ bins of the normalized differential cross section as a function of $\cos\theta^{\star}_{\ell^+} \cos\theta^{\star}_{\ell^-}$ and $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t65
title: "Table 65" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Values of $A_{P}$ in the 3 bins of $p_\mathrm{T}^\mathrm{t\bar{t}}$, and inclusively (bottom row). The value 9999 is used as a placeholder for infinity.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t66
title: "Table 66" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Statistical correlation matrix for $A_{P}$ in the 3 bins of $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t67
title: "Table 67" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Systematic correlation matrix for $A_{P}$ in the 3 bins of $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t68
title: "Table 68" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Fraction of events in each of the $6\times3$ bins of the normalized differential cross section as a function of $\cos\theta^{\star}_\ell$ and $p_\mathrm{T}^\mathrm{t\bar{t}}$. The value 9999 is used as a placeholder for infinity.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t69
title: "Table 69" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Statistical covariance matrix for the $6\times3$ bins of the normalized differential cross section as a function of $\cos\theta^{\star}_\ell$ and $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.17182/hepdata.70879.v1/t70
title: "Table 70" of "Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV"

description: Systematic covariance matrix for the $6\times3$ bins of the normalized differential cross section as a function of $\cos\theta^{\star}_\ell$ and $p_\mathrm{T}^\mathrm{t\bar{t}}$.
description: Measurements of the top quark-antiquark ($\mathrm{t\bar{t}}$) spin correlations and the top quark polarization are presented for $\mathrm{t\bar{t}}$ pairs produced in pp collisions at $\sqrt{s}=8\:$TeV. The data correspond to an integrated luminosity of 19.5 inverse-femtobarns collected with the CMS detector at the LHC. The measurements are performed using events with two oppositely charged leptons (electrons or muons) and two or more jets, where at least one of the jets is identified as originating from a bottom quark. The spin correlations and polarization are measured from the angular distributions of the two selected leptons, both inclusively and differentially, with respect to the invariant mass, rapidity, and transverse momentum of the $\mathrm{t\bar{t}}$ system. The measurements are unfolded to the parton level and found to be in agreement with predictions of the standard model. A search for new physics in the form of anomalous top quark chromo moments is performed. No evidence of new physics is observed, and exclusion limits on the real part of the chromo-magnetic dipole moment and the imaginary part of the chromo-electric dipole moment are evaluated.

For the normalized differential cross sections as a function of the angular variables the distributions are normalized to unit area, i.e. the bin values (and their associated covariances) should be multiplied by the bin widths to give the fraction of events in that bin. For the normalized double-differential cross sections as a function of the angular variables and the $\mathrm{t\bar{t}}$ system variables, the quoted bin values (and their associated covariances) are for the fraction of events in that bin, such that the sum of all bin contents is equal to one.

Bin values are reported to four decimal places, and covariances to four significant figures. Any missing figures are zeros.
DOI: 10.5281/zenodo.15491619
title: Geomagnetic Field, Impedance Tensor and Hall Prode GIC data from 2024-04-23 in AB, Canada

description: This data product consists of magnetic field, impedance and geomagnetically induced current (GIC) data. This data was analyzed and presented in the paper "The influence of 3-D Earth Conductivity, Geoelectric Field Polarization, and Power Grid Topology on GIC risk." See Parry et al., 2025 (Space Weather).

Magnetic Data (Magnetic_Data.zip): Geomagnetic data from April 24, 2023, from three CARISMA magnetometer stations in Alberta, Canada: Fort Chipewyan (FCHP), Fort MacMurray (MCMU), and Ministik Lake (MSTK). Raw data are from CARISMA (www.carisma.ca)

Magnetotelluric Data (MT_Data.zip): Includes magnetotelluric data collected by Martyn Unsworth's group at the University of Alberta over the last 20 years, as well as some older LITHOPROBE sites(AB_BC_MT_DATA_526_sites_230321.mat). Similar versions of this data set were previously published in: https://doi.org/10.5281/zenodo.10594300. Text files for the impedance tenors at three particular MT stations (abt500, abt272, and nab944RR940) are also included. 

GIC Data (20230424_hallprobe_data.mat): The GIC data file includes the UT time (GMT+6 = Mountain Daylight Time) and the transformer neutral-to-ground current data measured at two substations in central Alberta on 2023-04-24. See Parry et al., 2025 (Space Weather), for more details.
DOI: 10.6084/m9.figshare.29142482
title: Dataset_NephroLongCovid_figshare.xlsx

description: The aim of this study was to identify ME/CFS patients among Long-Covid patients with elevated autoantibodies. In 7 cases plasmapheresis (PE) and intravenous immunoglobulins (IVIG) with repetitive autoantibody-measurements were applied: 4 PE sessions on day 1, 5, 30 and 60 and a low-dose IVIG therapy after each treatment. Antibodies were measured before the first PE, and two weeks after the last PE session. To monitor clinical outcomes, somatic and psychometric follow-up assessments were conducted before the first PE, 2 weeks after the second, and 2 weeks after the last PE: Schellong test, ISI (insomnia), FSS (fatigue), HADS (depression and anxiety), and EQ-5D-5L (quality of life) questionnaires.
DOI: 10.1184/r1/29104236
title: Labeled_AAV8_Capsid_Data

description: <b>Data & File Overview</b><b>Directory of Files</b>:<b><i>All_Patches_resized.zip</i></b><b>Size</b>: (9.44GB)<b>Description</b>:<br>This is a compressed folder that contains preprocessed patches. Each patch is an image of one of the following classes:full capsidpartially full capsidempty capsidaggregationicebroken capsidbackground<b>names_labels_df.csv.zip</b><b>Size</b>: (293KB)<b>Description</b>:<br>This is a compressed .csv file that contains 94,830 patch instances each with a patch name and the associated class label.<b>Additional Notes:</b>This data was used in conjunction with the code at https://github.com/lcgutier/capsid-eyes to create the Capsidize app at https://github.com/lcgutier/Capsidize.<b>File Naming Convention</b>:<b>Annotated and Preprocessed Images</b>:The classes are defined as follows: 1=Full capsid, 2=Partially full capsid, 3=empty capsid, 4=aggregation, 5=ice, 6=broken capsid, 7=background Training and testing sets were randomly sampled from the resulting patches and each class was balanced.Images are named according to the dataset they belong to, followed by the original image ID number and lastly with the annotation ID number.<b>Data Description</b><b>names_labels_df.csv.zip</b><b>Columns</b>: patch_name, label<b>Rows</b>: 94,830 patch instances<b>Class Types</b><b>Full Capsids</b>, <b>label</b>=1, <b>Description</b>: A capsid with a dark ring and even dark infill density.<b>Partial Capsids</b>, <b>label</b>=2, <b>Description</b>: A capsid with a dark ring and a mid-range infill density.<b>Empty Capsids</b>, <b>label</b>=3, <b>Description</b>: A capsid with a dark ring and a light infill density.<b>Aggregation</b>, <b>label</b>=4, <b>Description</b>: A cluster of capsids.<b>Ice</b>, <b>label</b>=5, <b>Description</b>: Dark globular crystals that range in size.<b>Broken Capsids</b>, <b>label</b>=6, <b>Description</b>: Full, partial, or empty capsids that have broken. These are often only fragments.<b>Background</b>, <b>label</b>=7, <b>Description</b>: This class contains all background masks including those as a result of background differences seen at the carbon grid hole/grid material boundary.<b>Methodological Information</b><b>Software-specific information</b>:<b>Name</b>: Capsidize<b>Version</b>: 1.0.0<b>System Requirements</b>: Macos or Python 3.9<b>Open Source</b>: Yes<b>Developer</b>: Lilianna GutierrezProduct RepositorySource RepositoryAdditional Notes: The source code held in the capsid-eyes github repository can be run without macos, but the app was compiled on darwin-arm64.<b>Equipment-specific information</b>:<br><b>Sample Preparation</b><b>Manufacturer</b>: (Thermo Fisher Scientific [TFS], Waltham, MA, USA)<b>Model</b>: Vitrobot Mk 4<b>Use</b>: cooled in a bath of liquid nitrogen to freeze samples for imaging<b>Imaging</b><b>Manufacturer</b>: Thermo Fisher Scientific<b>Model</b>: Krios 3Gi microscope<b>Use</b>: To collect TEM images. Operating at 300 kVolts and equipped with a Selectris energy filter and Falcon 4i direct electron detecting camera operating in electron counting mode.
DOI: 10.15468/dl.w6csbd
title: Occurrence Download

description: A dataset containing 5454 species occurrences available in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is Human Observation",
 "Country is Mexico",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "TaxonKey is Iguana iguana (Linnaeus, 1758)",
 "Year 2020-2025"
 ]
}

 The dataset includes 5454 records from 6 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0016013-250515123054153/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.22003/xfel.eu-data-009216-00
title: Finalization of the characterization of the oxygen release compound HPBC