cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.57625.v1/t14
title: "Table 14" of "Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy"

description: 3-to-2 jet differential cross section ratio as a function of the leading jet PT with R=0.4 for a minimum non-leading jet PT of 80 GeV. Also tabulated are the theoretical values from a NLO pQCD calculation with total systematic error.
description: CERN-LHC. Study of inclusive multi-jet production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample was collected from April to August 2010 and has a total integrated luminosity of 2.4 pb^{-1} with a 3.4% uncertainty. Jets are identified using the anti-KT algorithm with results given for both R=0.4 and R=0.6. Jet multiplicities and differential cross sections are presented together with various ratios. The data are compared to Monte-Carlo predictions. In the tables where two systematic (sys) errors are shown, the first is the uncertainty on the jet energy scale and the second is the unfolding uncertainty. 

Note added (26 JUN 2014):
The cross section values reported in Tables 1, 3-9 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57625.v1/t15
title: "Table 15" of "Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy"

description: 3-to-2 jet differential cross section ratio as a function of the leading jet PT with R=0.4 for a minimum non-leading jet PT of 110 GeV. Also tabulated are the theoretical values from a NLO pQCD calculation with total systematic error.
description: CERN-LHC. Study of inclusive multi-jet production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample was collected from April to August 2010 and has a total integrated luminosity of 2.4 pb^{-1} with a 3.4% uncertainty. Jets are identified using the anti-KT algorithm with results given for both R=0.4 and R=0.6. Jet multiplicities and differential cross sections are presented together with various ratios. The data are compared to Monte-Carlo predictions. In the tables where two systematic (sys) errors are shown, the first is the uncertainty on the jet energy scale and the second is the unfolding uncertainty. 

Note added (26 JUN 2014):
The cross section values reported in Tables 1, 3-9 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57625.v1/t16
title: "Table 16" of "Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy"

description: 3-to-2 jet differential cross section ratio as a function of the sum of the PTs of the two leading jets with R=0.6. Also tabulated are the theoretical values from a NLO pQCD calculation with total systematic error.
description: CERN-LHC. Study of inclusive multi-jet production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample was collected from April to August 2010 and has a total integrated luminosity of 2.4 pb^{-1} with a 3.4% uncertainty. Jets are identified using the anti-KT algorithm with results given for both R=0.4 and R=0.6. Jet multiplicities and differential cross sections are presented together with various ratios. The data are compared to Monte-Carlo predictions. In the tables where two systematic (sys) errors are shown, the first is the uncertainty on the jet energy scale and the second is the unfolding uncertainty. 

Note added (26 JUN 2014):
The cross section values reported in Tables 1, 3-9 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57625.v1/t17
title: "Table 17" of "Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy"

description: 3-to-2 jet differential cross section ratio as a function of the sum of the PTs of the two leading jets with R=0.4. Also tabulated are the theoretical values from a NLO pQCD calculation with total systematic error.
description: CERN-LHC. Study of inclusive multi-jet production in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample was collected from April to August 2010 and has a total integrated luminosity of 2.4 pb^{-1} with a 3.4% uncertainty. Jets are identified using the anti-KT algorithm with results given for both R=0.4 and R=0.6. Jet multiplicities and differential cross sections are presented together with various ratios. The data are compared to Monte-Carlo predictions. In the tables where two systematic (sys) errors are shown, the first is the uncertainty on the jet energy scale and the second is the unfolding uncertainty. 

Note added (26 JUN 2014):
The cross section values reported in Tables 1, 3-9 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57626.v1/t1
title: "Table 1" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [1,2], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t2
title: "Table 2" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [2,3], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t3
title: "Table 3" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [3,4], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t4
title: "Table 4" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [4,5], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t10
title: "Table 10" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [180,210] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t11
title: "Table 11" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [210,240] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t5
title: "Table 5" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the mean transverse momentum of the boundary jets for boundary jets having a rapidity difference in the range [5,6], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t6
title: "Table 6" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [70,90] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t7
title: "Table 7" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [90,120] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t8
title: "Table 8" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [120,150] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t9
title: "Table 9" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [150,180] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.
DOI: 10.17182/hepdata.57626.v1/t12
title: "Table 12" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector"

description: The Gap Fraction as a function of the rapidity difference between the two boundary jets for boundary jets having a mean transverse momentum in the range [240,270] GeV, using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
description: CERN-LHC. Measurement of dijet production with a jet veto on additional central jet activity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The measurement was performed using 2010 data recorded by the ATLAS detector. The boundary jets system is defined using two different selection criteria: the two leading pT jets selection, where the two highest transverse momentum jets (of transverse momentum pT &gt; 20 GeV and absolute rapidity |y| &lt; 4.4) in the events are used and the forward-backward selection, where the most forward and most backward jets in the events (same selection cuts) are used. The Gap Fraction is defined as the fraction of dijet events which have no other jets with transverse momentum above a veto scale Q0 (20 GeV) in the rapidity interval between the boundary jets. Also measured is the mean multiplicity of jets above this veto scale in the rapidity interval bounded by the dijet system.