cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.67531.v2/t117
title: "Table 117" of "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC"

description: Raa in different eta intervals (not shown in Fig. 18).
description: CERN-LHC. Charged-particle spectra obtained in 0.15 nb${}^{-1}$ of Pb+Pb interactions at $\sqrt{{s}_\mathsf{{NN}}}=2.76$TeV and 4.2 pb${}^{-1}$ of pp interactions at $\sqrt{s}=2.76$ TeV with the ATLAS detector at the LHC are presented in a wide transverse momentum ($0.5 &lt; p_{\mathrm{T}} &lt; 150$ GeV) and pseudorapidity ($|\eta|&lt;2$) range. For Pb+Pb collisions, the spectra are presented as a function of collision centrality, which is determined by the response of the forward calorimeter located on both sides of the interaction point. The nuclear modification factors $R_{\mathrm{AA}}$ and $R_{\mathrm{CP}}$ are presented in detail as function of centrality, $p_{\mathrm{T}}$ and $\eta$. They show a distinct $p_{\mathrm{T}}$-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, $R_{\mathrm{AA}}$ is consistent with a plateau at a centrality-dependent value, within the uncertainties. The value is $0.55\pm0.01(stat.)\pm0.04(syst.)$ in the most central collisions. The $R_{\mathrm{AA}}$ distribution is consistent with flat $|\eta|$ dependence over the whole transverse momentum range in all centrality classes.
DOI: 10.25934/pr00011752
title: Prospective Open-Label Study of Pharmacokinetics, Efficacy and Safety of Immune Globulin Intravenous (Human), 10% TVR Solution in Patients With Hypo- or Agammaglobulinemia

description: The purpose of this study is to determine the pharmacokinetics, efficacy and safety of Immune Globulin Intravenous (Human), 10% TVR (Triple Virally Reduced) Solution in subjects with primary immunodeficiency (PID) manifesting as hypo- or agammaglobulinemia. Subjects are treated every 21 days and receive a total of 12 infusions: for the first 3 infusions subjects receive GAMMAGARD S/D to ensure a steady-state and to acquire data with a licensed product; for the remaining 9 infusions subjects receive IGIV, 10% TVR Solution.
DOI: 10.17182/hepdata.67531.v2/t118
title: "Table 118" of "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC"

description: Raa in different eta intervals.
description: CERN-LHC. Charged-particle spectra obtained in 0.15 nb${}^{-1}$ of Pb+Pb interactions at $\sqrt{{s}_\mathsf{{NN}}}=2.76$TeV and 4.2 pb${}^{-1}$ of pp interactions at $\sqrt{s}=2.76$ TeV with the ATLAS detector at the LHC are presented in a wide transverse momentum ($0.5 &lt; p_{\mathrm{T}} &lt; 150$ GeV) and pseudorapidity ($|\eta|&lt;2$) range. For Pb+Pb collisions, the spectra are presented as a function of collision centrality, which is determined by the response of the forward calorimeter located on both sides of the interaction point. The nuclear modification factors $R_{\mathrm{AA}}$ and $R_{\mathrm{CP}}$ are presented in detail as function of centrality, $p_{\mathrm{T}}$ and $\eta$. They show a distinct $p_{\mathrm{T}}$-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, $R_{\mathrm{AA}}$ is consistent with a plateau at a centrality-dependent value, within the uncertainties. The value is $0.55\pm0.01(stat.)\pm0.04(syst.)$ in the most central collisions. The $R_{\mathrm{AA}}$ distribution is consistent with flat $|\eta|$ dependence over the whole transverse momentum range in all centrality classes.
DOI: 10.17182/hepdata.67531.v2/t119
title: "Table 119" of "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC"

description: Raa in different eta intervals (not shown in Fig. 18).
description: CERN-LHC. Charged-particle spectra obtained in 0.15 nb${}^{-1}$ of Pb+Pb interactions at $\sqrt{{s}_\mathsf{{NN}}}=2.76$TeV and 4.2 pb${}^{-1}$ of pp interactions at $\sqrt{s}=2.76$ TeV with the ATLAS detector at the LHC are presented in a wide transverse momentum ($0.5 &lt; p_{\mathrm{T}} &lt; 150$ GeV) and pseudorapidity ($|\eta|&lt;2$) range. For Pb+Pb collisions, the spectra are presented as a function of collision centrality, which is determined by the response of the forward calorimeter located on both sides of the interaction point. The nuclear modification factors $R_{\mathrm{AA}}$ and $R_{\mathrm{CP}}$ are presented in detail as function of centrality, $p_{\mathrm{T}}$ and $\eta$. They show a distinct $p_{\mathrm{T}}$-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, $R_{\mathrm{AA}}$ is consistent with a plateau at a centrality-dependent value, within the uncertainties. The value is $0.55\pm0.01(stat.)\pm0.04(syst.)$ in the most central collisions. The $R_{\mathrm{AA}}$ distribution is consistent with flat $|\eta|$ dependence over the whole transverse momentum range in all centrality classes.
DOI: 10.17182/hepdata.67531.v2/t120
title: "Table 120" of "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC"

description: Raa in different eta intervals.
description: CERN-LHC. Charged-particle spectra obtained in 0.15 nb${}^{-1}$ of Pb+Pb interactions at $\sqrt{{s}_\mathsf{{NN}}}=2.76$TeV and 4.2 pb${}^{-1}$ of pp interactions at $\sqrt{s}=2.76$ TeV with the ATLAS detector at the LHC are presented in a wide transverse momentum ($0.5 &lt; p_{\mathrm{T}} &lt; 150$ GeV) and pseudorapidity ($|\eta|&lt;2$) range. For Pb+Pb collisions, the spectra are presented as a function of collision centrality, which is determined by the response of the forward calorimeter located on both sides of the interaction point. The nuclear modification factors $R_{\mathrm{AA}}$ and $R_{\mathrm{CP}}$ are presented in detail as function of centrality, $p_{\mathrm{T}}$ and $\eta$. They show a distinct $p_{\mathrm{T}}$-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, $R_{\mathrm{AA}}$ is consistent with a plateau at a centrality-dependent value, within the uncertainties. The value is $0.55\pm0.01(stat.)\pm0.04(syst.)$ in the most central collisions. The $R_{\mathrm{AA}}$ distribution is consistent with flat $|\eta|$ dependence over the whole transverse momentum range in all centrality classes.
DOI: 10.17182/hepdata.67531.v2/t121
title: "Table 121" of "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC"

description: Raa in different eta intervals.
description: CERN-LHC. Charged-particle spectra obtained in 0.15 nb${}^{-1}$ of Pb+Pb interactions at $\sqrt{{s}_\mathsf{{NN}}}=2.76$TeV and 4.2 pb${}^{-1}$ of pp interactions at $\sqrt{s}=2.76$ TeV with the ATLAS detector at the LHC are presented in a wide transverse momentum ($0.5 &lt; p_{\mathrm{T}} &lt; 150$ GeV) and pseudorapidity ($|\eta|&lt;2$) range. For Pb+Pb collisions, the spectra are presented as a function of collision centrality, which is determined by the response of the forward calorimeter located on both sides of the interaction point. The nuclear modification factors $R_{\mathrm{AA}}$ and $R_{\mathrm{CP}}$ are presented in detail as function of centrality, $p_{\mathrm{T}}$ and $\eta$. They show a distinct $p_{\mathrm{T}}$-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, $R_{\mathrm{AA}}$ is consistent with a plateau at a centrality-dependent value, within the uncertainties. The value is $0.55\pm0.01(stat.)\pm0.04(syst.)$ in the most central collisions. The $R_{\mathrm{AA}}$ distribution is consistent with flat $|\eta|$ dependence over the whole transverse momentum range in all centrality classes.
DOI: 10.17182/hepdata.67634.v1/t1
title: "Table 1" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dET in pb/GeV. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t2
title: "Table 2" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dET in pb/GeV given (0.05 &lt; DeltaR &lt; 0.5). For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t3
title: "Table 3" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dET in pb/GeV given (0.5 &lt; DeltaR &lt; 3.0). For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.25934/pr00011753
title: A Clinical Investigation to Assess the Safety and Efficacy of Immune Globulin Intravenous (Human), 10% in Subjects With Primary Immunodeficiency Disorders

description: The purpose of this study is to assess the safety and efficacy of Immune Globulin Intravenous (Human), 10% (IGIV 10%) in subjects with primary immunodeficiency disorders.
DOI: 10.17182/hepdata.67634.v1/t4
title: "Table 4" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dET in pb/GeV given q_T &lt; 10 GeV. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t5
title: "Table 5" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dET in pb/GeV given q_T &gt; 50 GeV. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t6
title: "Table 6" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dDR in pb/radians. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t7
title: "Table 7" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dDR in pb/radians given q_T &lt; 10 GeV. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67634.v1/t8
title: "Table 8" of "A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV"

description: Measured differential cross section dsigma/dDR in pb/radians given q_T &gt; 50 GeV. For the data values, the first
uncertainty is statistical and the second is systematic. For the theory values, the uncertainty
combines statistical, PDF, and renormalization/factorization scale components.
description: CERN-LHC. The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as 
a function of the transverse energy of the photon and its separation from the nearest muon. The data for these 
measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns 
of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC.

These cross sections are given for the fiducial region defined as follows:
- Leading muon p_T &gt; 31 GeV and abs(eta) &lt; 2.4
- Trailing muon p_T &gt; 9 GeV and abs(eta) &lt; 2.4
- Photon p_T &gt; 5 GeV
- Photon abs(eta) &lt; 2.4 but not 1.4 &lt; abs(eta) &lt; 1.6
- Separation between photon and closest muon 0.05 &lt; DeltaR &lt; 3.0
- Di-muon invariant mass 30 &lt; M_mumu &lt; 87 GeV.
DOI: 10.17182/hepdata.67635.v1/t1
title: "Table 1" of "Measurements of jet multiplicity and differential production cross sections of Z+jets events in proton-proton collisions at sqrt(s)=7 TeV"

description: The cross section measurement as a function of the exclusive jet multiplicity, for jet multiplicities of up to 6.
description: CERN-LHC. Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at sqrt(s) = 7 TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 fb^-1. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD.

The data tables are provided rounded with respect to what is used in RIVET.
DOI: 10.17182/hepdata.67635.v1/t2
title: "Table 2" of "Measurements of jet multiplicity and differential production cross sections of Z+jets events in proton-proton collisions at sqrt(s)=7 TeV"

description: The cross section measurement as a function of the inclusive jet multiplicity, for jet multiplicities of up to 6.
description: CERN-LHC. Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at sqrt(s) = 7 TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 fb^-1. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD.

The data tables are provided rounded with respect to what is used in RIVET.
DOI: 10.17182/hepdata.67635.v1/t3
title: "Table 3" of "Measurements of jet multiplicity and differential production cross sections of Z+jets events in proton-proton collisions at sqrt(s)=7 TeV"

description: The cross section measurement as a function of the transverse momentum of the leading jet.
description: CERN-LHC. Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at sqrt(s) = 7 TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 fb^-1. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD.

The data tables are provided rounded with respect to what is used in RIVET.
DOI: 10.17182/hepdata.67635.v1/t4
title: "Table 4" of "Measurements of jet multiplicity and differential production cross sections of Z+jets events in proton-proton collisions at sqrt(s)=7 TeV"

description: The cross section measurement as a function of the transverse momentum of the second leading jet.
description: CERN-LHC. Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at sqrt(s) = 7 TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 fb^-1. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD.

The data tables are provided rounded with respect to what is used in RIVET.
DOI: 10.17182/hepdata.67635.v1/t5
title: "Table 5" of "Measurements of jet multiplicity and differential production cross sections of Z+jets events in proton-proton collisions at sqrt(s)=7 TeV"

description: The cross section measurement as a function of the transverse momentum of the third leading jet.
description: CERN-LHC. Measurements of differential cross sections are presented for the production of a Z boson and at least one hadronic jet in proton-proton collisions at sqrt(s) = 7 TeV, recorded by the CMS detector, using a data sample corresponding to an integrated luminosity of 4.9 fb^-1. The jet multiplicity distribution is measured for up to six jets. The differential cross sections are measured as a function of jet transverse momentum and pseudorapidity for the four highest transverse momentum jets. The distribution of the scalar sum of jet transverse momenta is also measured as a function of the jet multiplicity. The measurements are compared with theoretical predictions at leading and next-to-leading order in perturbative QCD.

The data tables are provided rounded with respect to what is used in RIVET.