cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.57626.v1/t13
title: "Table 13" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [70,90} GeV and rapidity difference in the range [2,3]. 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/t14
title: "Table 14" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [70,90} GeV and rapidity difference in the range [4,5]. 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/t15
title: "Table 15" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [120,150} GeV and rapidity difference in the range [2,3]. 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/t16
title: "Table 16" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [120,150} GeV and rapidity difference in the range [4,5]. 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/t17
title: "Table 17" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [210,240} GeV and rapidity difference in the range [2,3]. 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/t18
title: "Table 18" 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 dijet veto energy, Q0, for boundary jets having a mean transverse momentum in the range [210,240} GeV and rapidity difference in the range [4,5]. 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/t19
title: "Table 19" 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 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/t20
title: "Table 20" 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 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/t21
title: "Table 21" 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 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/t23
title: "Table 23" 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 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.55696.v1/t13
title: "Table 13" of "Differential cross sections and recoil polarizations for the reaction gamma p -&gt; K+ Sigma0"

description: Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.81 to 1.82 GeV.
description: Jefferson Lab. High statistics measurements of the differential cross section and recoil polarizations for the reaction GAMMA P --&gt; K+ SIGMA0. The data cover the centre-of-mass energy from 1.69 to 2.84 GeV and the extensive angular range in cos(theta(K+,CM)) from -0.95 to 0.95. Numerical values supplied by B Dey.
DOI: 10.17182/hepdata.55696.v1/t16
title: "Table 16" of "Differential cross sections and recoil polarizations for the reaction gamma p -&gt; K+ Sigma0"

description: Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.84 to 1.85 GeV.
description: Jefferson Lab. High statistics measurements of the differential cross section and recoil polarizations for the reaction GAMMA P --&gt; K+ SIGMA0. The data cover the centre-of-mass energy from 1.69 to 2.84 GeV and the extensive angular range in cos(theta(K+,CM)) from -0.95 to 0.95. Numerical values supplied by B Dey.
DOI: 10.17182/hepdata.55696.v1/t17
title: "Table 17" of "Differential cross sections and recoil polarizations for the reaction gamma p -&gt; K+ Sigma0"

description: Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.85 to 1.86 GeV.
description: Jefferson Lab. High statistics measurements of the differential cross section and recoil polarizations for the reaction GAMMA P --&gt; K+ SIGMA0. The data cover the centre-of-mass energy from 1.69 to 2.84 GeV and the extensive angular range in cos(theta(K+,CM)) from -0.95 to 0.95. Numerical values supplied by B Dey.
DOI: 10.17182/hepdata.55696.v1/t25
title: "Table 25" of "Differential cross sections and recoil polarizations for the reaction gamma p -&gt; K+ Sigma0"

description: Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.93 to 1.94 GeV.
description: Jefferson Lab. High statistics measurements of the differential cross section and recoil polarizations for the reaction GAMMA P --&gt; K+ SIGMA0. The data cover the centre-of-mass energy from 1.69 to 2.84 GeV and the extensive angular range in cos(theta(K+,CM)) from -0.95 to 0.95. Numerical values supplied by B Dey.
DOI: 10.17182/hepdata.55696.v1/t31
title: "Table 31" of "Differential cross sections and recoil polarizations for the reaction gamma p -&gt; K+ Sigma0"

description: Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2 to 2.01 GeV.
description: Jefferson Lab. High statistics measurements of the differential cross section and recoil polarizations for the reaction GAMMA P --&gt; K+ SIGMA0. The data cover the centre-of-mass energy from 1.69 to 2.84 GeV and the extensive angular range in cos(theta(K+,CM)) from -0.95 to 0.95. Numerical values supplied by B Dey.
DOI: 10.17182/hepdata.57626.v1/t22
title: "Table 22" 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 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/t24
title: "Table 24" 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 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/t25
title: "Table 25" 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 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/t26
title: "Table 26" 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 [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.