cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89321.v2/t182
title: "Table 182" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the average fragmentation function per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t183
title: "Table 183" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the average relative $p_T$ per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t184
title: "Table 184" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the average r per jet $p_T$ bin. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t185
title: "Table 185" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the number of tracks. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t186
title: "Table 186" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the fragmentation function. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t187
title: "Table 187" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the relative $p_T$. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89321.v2/t188
title: "Table 188" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The total uncertainty covariance matrix for the r. The first half of the bins on a given axis correspond to the more central jet while the second half correspond to the more forward jet. See Fig. 4 in the paper for more information about the binning. The covariance matrix is the sum of the covariance matrices for each source of systematic and statistical uncertainty. Note that the overall sign for the systematic uncertainty covariances is arbitrary.
description: CERN-LHC. 

This paper presents a measurement of quantities related to the formation of jets from high energy quarks and gluons (fragmentation). Jets with $100$ GeV $ 500$ MeV~and $|\eta| &lt; 2.5$~are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the leading two jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons to parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark- and gluon- extractions using simulation input. The simulations provide a reasonable description of the quark-like data across the jet $p_\text{T}$ range presented in this measurement, but the gluon-like data have systematically fewer charged particles than the simulations. Uncertainties are broken down by category and should be treated as fully correlated between bins and between observables except for statistical uncertainties.
DOI: 10.17182/hepdata.89322.v1/t1
title: "Table 2a" of "Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The correction factors, $C_{W^±,i}$ with their associated systematic uncertainties as a function of $|\eta_{\mu}|$, for $W^+$ and $W^−$
description: "Measurements of the $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ cross-sections
and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.
The data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV
with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\textrm{fb}^{-1}$.
The integrated cross-sections for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ production are measured in a fiducial phase space defined 
at the particle level by requiring the muon transverse momentum to be greater than 25 GeV 
and the neutrino transverse momentum to be greater than 25 GeV. 
The absolute muon pseudorapidity is required to be less than 2.4. 
The W boson transverse mass must be at least 40 GeV.
The differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. 
These are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at 
0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. 
See 1904.05631 for more details."
DOI: 10.17182/hepdata.89322.v1/t2
title: "Table 2b" of "Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The integrated global correction factor $C_{W^±}$, for $W^+$ and $W^−$
description: "Measurements of the $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ cross-sections
and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.
The data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV
with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\textrm{fb}^{-1}$.
The integrated cross-sections for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ production are measured in a fiducial phase space defined 
at the particle level by requiring the muon transverse momentum to be greater than 25 GeV 
and the neutrino transverse momentum to be greater than 25 GeV. 
The absolute muon pseudorapidity is required to be less than 2.4. 
The W boson transverse mass must be at least 40 GeV.
The differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. 
These are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at 
0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. 
See 1904.05631 for more details."
DOI: 10.15468/dl.m88jpb
title: Occurrence Download

description: A dataset containing 6223 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-73.84827 45.40769,-73.55825 45.42534,-73.4885 45.53938,-73.44989 45.6952,-73.45718 45.72988,-73.76763 45.58376,-74.01964 45.42439,-73.93719 45.3903,-73.84827 45.40769))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Chaetura pelagica",
 "Year 2023-2025"
 ]
}

 The dataset includes 6223 records from 5 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015488-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.89322.v1/t3
title: "Table 3" of "Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Cross-sections (differential in $\eta_{\mu}$) and asymmetry, as a function of $|\eta_{\mu}|$). The central values are provided along with the statistical and dominant systematic uncertainties: the data statistical uncertainty (Data Stat.), the $E_T^{\textrm{miss}}$ uncertainty, the uncertainties related to muon reconstruction (Muon Reco.), those related to the background, those from MC statistics (MC Stat.), and modelling uncertainties. The uncertainties of the cross-sections are given in percent and those of the asymmetry as an absolute difference from the nominal.
description: "Measurements of the $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ cross-sections
and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.
The data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV
with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\textrm{fb}^{-1}$.
The integrated cross-sections for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ production are measured in a fiducial phase space defined 
at the particle level by requiring the muon transverse momentum to be greater than 25 GeV 
and the neutrino transverse momentum to be greater than 25 GeV. 
The absolute muon pseudorapidity is required to be less than 2.4. 
The W boson transverse mass must be at least 40 GeV.
The differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. 
These are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at 
0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. 
See 1904.05631 for more details."
DOI: 10.17182/hepdata.89322.v1/t4
title: "Table 4a" of "Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The measured fiducial production cross-sections times branching ratio for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$, their sum, and their ratio for data
description: "Measurements of the $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ cross-sections
and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.
The data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV
with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\textrm{fb}^{-1}$.
The integrated cross-sections for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ production are measured in a fiducial phase space defined 
at the particle level by requiring the muon transverse momentum to be greater than 25 GeV 
and the neutrino transverse momentum to be greater than 25 GeV. 
The absolute muon pseudorapidity is required to be less than 2.4. 
The W boson transverse mass must be at least 40 GeV.
The differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. 
These are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at 
0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. 
See 1904.05631 for more details."
DOI: 10.17182/hepdata.89322.v1/t5
title: "Table 4b" of "Measurement of the cross-section and charge asymmetry of $W$ bosons produced in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The measured fiducial production cross-sections times branching ratio for $W^+\rightarrow\mu^+
u$ and $W^-\rightarrow\mu^-\bar{\nu}$, their sum, and their ratio for the predictions from DYNNLO (CT14 NNLO PDF set)
description: "Measurements of the $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ cross-sections
and the associated charge asymmetry as a function of the absolute pseudorapidity of the decay muon.
The data were collected in proton-proton collisions at a centre-of-mass energy of 8 TeV
with the ATLAS experiment at the LHC and correspond to a total integrated luminosity of 20.2 $\textrm{fb}^{-1}$.
The integrated cross-sections for $W^+\rightarrow\mu^+\nu$ and $W^-\rightarrow\mu^-\bar{\nu}$ production are measured in a fiducial phase space defined 
at the particle level by requiring the muon transverse momentum to be greater than 25 GeV 
and the neutrino transverse momentum to be greater than 25 GeV. 
The absolute muon pseudorapidity is required to be less than 2.4. 
The W boson transverse mass must be at least 40 GeV.
The differential cross-sections and charge asymmetry are measured in the same fiducial phase space as for the integrated measurement. 
These are measured in 11 bins of absolute muon pseudorapidity between 0 and 2.4 with bin edges at 
0, 0.21, 0.42, 0.63, 0.84, 1.05, 1.37, 1.52, 1.74, 1.95, 2.18, and 2.4. 
See 1904.05631 for more details."