cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.15468/dl.a2bnh3
title: Occurrence Download

description: A dataset containing 301 species occurrences available in GBIF matching the query:
{
 "and" : [
 "GadmGid is NPL",
 "OccurrenceStatus is Present",
 "TaxonKey is Panthera tigris"
 ]
}

 The dataset includes 301 records from 6 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015300-260129131611470/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.132904.v1/t1
title: "Table 1" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of jet double differential cross section in pp collisions at 5.02 TeV as a function of pT in bins of rg. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t2
title: "Table 2" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of jet double differential cross section in pp collisions at 5.02 TeV as a function of rg in bins of pT. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t3
title: "Table 3" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of pT in bins of rg for 50-80% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t4
title: "Table 4" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of pT in bins of rg for 30-50% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t5
title: "Table 5" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of pT in bins of rg for 10-30% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t6
title: "Table 6" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of pT in bins of rg for 0-10% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.15468/dl.ufysg9
title: Occurrence Download

description: A dataset containing 26782 species occurrences available in GBIF matching the query:
{
 "DatasetKey" : [
 "is EDIA – Global Bird Monitoring Program of the Alqueva Dam (EFMA) Secondary Irrigation Network (block B: irrigation blocks of Alfundão, Ferreira-Valbom, Loureiro-Alvito, Monte Novo, Pedrógão, Pisão, São Matias and Vale de Gaio): Bird Atlas - distributions [winter 2019 - spring 2020]"
 ]
}

 The dataset includes 26782 records from 1 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015299-260129131611470/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.132904.v1/t7
title: "Table 7" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of rg in bins of pT for 50-80% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t8
title: "Table 8" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of rg in bins of pT for 30-50% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t9
title: "Table 9" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of rg in bins of pT for 10-30% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t10
title: "Table 10" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of per-event jet yields in Pb+Pb collisions at 5.02 TeV as a function of rg in bins of pT for 0-10% centrality interval, normalized by the respective centrality interval's . Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t11
title: "Table 11" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of pT and in bins of rg for 50-80% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t12
title: "Table 12" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of pT and in bins of rg for 30-50% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t13
title: "Table 13" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of pT and in bins of rg for 10-30% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.