cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.57626.v1/t27
title: "Table 27" 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 mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have 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/t28
title: "Table 28" 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 mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have 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/t29
title: "Table 29" 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 mean number of jets in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have 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/t30
title: "Table 30" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [70,90] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t31
title: "Table 31" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [90,120] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t32
title: "Table 32" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [120,150] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t33
title: "Table 33" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [150,180] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t34
title: "Table 34" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [180,210] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t35
title: "Table 35" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [210,240] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t36
title: "Table 36" 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 mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [240,270] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
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/t37
title: "Table 37" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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/t38
title: "Table 38" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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/t39
title: "Table 39" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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/t41
title: "Table 41" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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/t42
title: "Table 42" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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/t40
title: "Table 40" 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 mean number of jets as a function of the rapidity difference between the two boundary jets for boundary jets that have 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.