cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.68020.v1/t13
title: "Table 13" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 0 &lt; |y| &lt; 0.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t14
title: "Table 14" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 0.5 &lt; |y| &lt; 1. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t15
title: "Table 15" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 1 &lt; |y| &lt; 1.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t16
title: "Table 16" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 1.5 &lt; |y| &lt; 2. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t17
title: "Table 17" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 2 &lt; |y| &lt; 2.5. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68020.v1/t18
title: "Table 18" of "Measurement of the ratio of inclusive jet cross sections using the anti-kt algorithm with radius parameters R = 0.5 and 0.7 in pp collisions at sqrt(s) = 7 TeV"

description: Jet radius ratio R(0.5, 0.7) in the rapidity bin 2.5 &lt; |y| &lt; 3. The total uncorrelated uncertainty includes statistical one and systematic uncorrelated. The total systematic uncertainty includes all other sources. The total error can be obtained as a quadratic sum of uncorrelated and correlated one. The NP correction can be used to scale theory prediction to compare to data at particle level.
description: CERN-LHC. Measurements of the inclusive jet cross section with the anti-kt clustering algorithm are presented for two radius parameters, R=0.5 and 0.7. They are based on data from LHC proton-proton collisions at $\sqrt{s}$ = 7 TeV corresponding to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector in 2011. The ratio of these two measurements is obtained as a function of the rapidity and transverse momentum of the jets. Significant discrepancies are found comparing the data to leading-order simulations and to fixed-order calculations at next-to-leading order, corrected for nonperturbative effects, whereas simulations with next-to-leading-order matrix elements matched to parton showers describe the data best.
DOI: 10.17182/hepdata.68039.v1/t1
title: "Table 1" of "Measurement of the WZ production cross section and limits on anomalous triple gauge couplings in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: Total fiducial cross-section $WZ\to\ell\nu\ell\ell$.
description: CERN-LHC. This Letter presents a measurement of WZ production in 1.02 fb^-1 of pp collision data at sqrt(s) = 7 TeV collected by the ATLAS experiment in 2011. Doubly leptonic decay events are selected with electrons, muons and missing transverse momentum in the final state. In total 71 candidates are observed, with a background expectation of 12.1 +/- 1.4(stat.) +4.1/-2.0(syst) events. The total cross section for WZ production for Z gamma^* masses within the range 66 GeV to 116 GeV is determined to be sigma_WZ^tot = 20.5 +3.1/-2.8(stat.) +1.4/-1.3(syst.) +0.9/-0.8(lumi.)pb, which is consistent with the Standard Model expectation of 17.3 +1.3/-0.8 pb. Limits on anomalous triple gauge boson couplings are extracted.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t1
title: "Table 1" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;1$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t2
title: "Table 2" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;1$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t3
title: "Table 3" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t4
title: "Table 4" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t5
title: "Table 5" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t6
title: "Table 6" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t11
title: "Table 11" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t7
title: "Table 7" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;1$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t8
title: "Table 8" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;1$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t9
title: "Table 9" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 900$ GeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t10
title: "Table 10" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t12
title: "Table 12" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 500 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t13
title: "Table 13" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 100 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.
DOI: 10.17182/hepdata.68040.v1/t14
title: "Table 14" of "Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector"

description: $\sqrt{s} = 7$ TeV, $p_T &gt; 200 $ MeV, $|\eta|&lt;2.5$.
description: CERN-LHC. Using inelastic proton-proton interactions at sqrt(s) = 900 GeV and 7 TeV, recorded by the ATLAS detector at the LHC, measurements have been made of the correlations between forward and backward charged-particle multiplicities and, for the first time, between forward and backward charged-particle summed transverse momentum. In addition, jet-like structure in the events is studied by means of azimuthal distributions of charged particles relative to the charged particle with highest transverse momentum in a selected kinematic region of the event. The results are compared with predictions from tunes of the PYTHIA and HERWIG++ Monte Carlo generators, which in most cases are found to provide a reasonable description of the data.
Data taken from the RIVET analysis code.