cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95241.v1/t69
title: "Table 69" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 84 &lt; p_{T} &lt; 97 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t70
title: "Table 70" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 97 &lt; p_{T} &lt; 133 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t71
title: "Table 71" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 133 &lt; p_{T} &lt; 196 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t72
title: "Table 72" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 196 &lt; p_{T} &lt; 272 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t73
title: "Table 73" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 272 &lt; p_{T} &lt; 330 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t74
title: "Table 74" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 330 &lt; p_{T} &lt; 395 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t75
title: "Table 75" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 395 &lt; p_{T} &lt; 468 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t76
title: "Table 76" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 468 &lt; p_{T} &lt; 548 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t77
title: "Table 77" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 548 &lt; p_{T} &lt; 638 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t78
title: "Table 78" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.0&lt;|y|&lt;1.5 and PT 638 &lt; p_{T} &lt; 1588 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t79
title: "Table 79" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 84 &lt; p_{T} &lt; 97 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t80
title: "Table 80" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 97 &lt; p_{T} &lt; 133 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t81
title: "Table 81" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 133 &lt; p_{T} &lt; 196 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t82
title: "Table 82" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 196 &lt; p_{T} &lt; 272 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t83
title: "Table 83" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 272 &lt; p_{T} &lt; 330 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t84
title: "Table 84" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 330 &lt; p_{T} &lt; 395 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t85
title: "Table 85" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 395 &lt; p_{T} &lt; 468 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t86
title: "Table 86" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 468 &lt; p_{T} &lt; 548 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t87
title: "Table 87" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 548 &lt; p_{T} &lt; 638 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95241.v1/t88
title: "Table 88" of "Dependence of inclusive jet production on the anti-$k_\mathrm{T}$ distance parameter in pp collisions at $\sqrt{s} =$ 13 TeV"

description: Ratio of cross section of inclusive anti-KT jets with respect to AK4 jets as a function of jet size in the rapidity range 1.5&lt;|y|&lt;2.0 and PT 638 &lt; p_{T} &lt; 1588 GeV. The nonperturbative correction can be used to scale fixed-order theory prediction to compare to data at particle level.
description: No description provided.
DOI: 10.17182/hepdata.95243.v1/t1
title: "Table 1" of "Observation of electroweak production of W$\gamma$ with two jets in proton-proton collisions at $\sqrt{s}= $ 13 TeV"

description: The measured EW W$\gamma$jj fiducial cross section. The uncertainty is the combined stastical uncertianty and the systematic uncertainty including experimental and theortical sources. The EW W$\gamma$jj is produced using MadGraph5_aMC@NLO v2.6.0 at LO. Within the acceptance, the theoretical cross section is 17.0 fb.
description: CERN-LHC. Measurement of the cross section for electroweak production and constraints on anomalous quartic couplings from events with a W boson and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV. The W boson candidates are selected through their decay into a electron or muon and corresponding neutrino. The process of interest, electroweak W gamma jj production, is isolated by selecting events with a large dijet mass and a large pseudorapidity gap between the two jets. The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1. The observed significance of the signal is 4.9 standard deviations, where a significance of 4.6 standard deviations is expected in the standard model predictions. The results are combined with previously published CMS results based on sqrt(s)=8 TeV data, which leads to an observed (expected) significance of 5.3 (4.8) standard deviations. The measured value of the fiducial cross section for the signal is reported. Bounds are given on quartic vector boson interactions in the framework of dimension-8 effective field theory operators at 95% confidence level.
DOI: 10.17182/hepdata.95243.v1/t2
title: "Table 2" of "Observation of electroweak production of W$\gamma$ with two jets in proton-proton collisions at $\sqrt{s}= $ 13 TeV"

description: The measured W$\gamma$jj cross section, combining the EW and QCD-induced production mechanisms. The uncertainty is the combined stastical uncertianty and the systematic uncertainty including experimental and theortical sources. The QCD W$\gamma$jj is produced using MadGraph5_aMC@NLO v2.4.2 at NLO in QCD. Within the acceptance, the theoretical cross section of QCD W$\gamma$jj is 72.7 fb. The EW W$\gamma$jj is produced using MadGraph5_aMC@NLO v2.6.0 at LO. Within the acceptance, the theoretical cross section of EW W$\gamma$jj is 17.0 fb. The total EW+QCD W$\gamma$ jj cross section is the sum of the two processes.
description: CERN-LHC. Measurement of the cross section for electroweak production and constraints on anomalous quartic couplings from events with a W boson and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV. The W boson candidates are selected through their decay into a electron or muon and corresponding neutrino. The process of interest, electroweak W gamma jj production, is isolated by selecting events with a large dijet mass and a large pseudorapidity gap between the two jets. The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1. The observed significance of the signal is 4.9 standard deviations, where a significance of 4.6 standard deviations is expected in the standard model predictions. The results are combined with previously published CMS results based on sqrt(s)=8 TeV data, which leads to an observed (expected) significance of 5.3 (4.8) standard deviations. The measured value of the fiducial cross section for the signal is reported. Bounds are given on quartic vector boson interactions in the framework of dimension-8 effective field theory operators at 95% confidence level.
DOI: 10.17182/hepdata.95243.v1/t3
title: "Table 3" of "Observation of electroweak production of W$\gamma$ with two jets in proton-proton collisions at $\sqrt{s}= $ 13 TeV"

description: Constraints on dimension-8 effective field theory operators.
description: CERN-LHC. Measurement of the cross section for electroweak production and constraints on anomalous quartic couplings from events with a W boson and a photon in association with two jets in proton-proton collisions at sqrt(s) = 13 TeV. The W boson candidates are selected through their decay into a electron or muon and corresponding neutrino. The process of interest, electroweak W gamma jj production, is isolated by selecting events with a large dijet mass and a large pseudorapidity gap between the two jets. The measurement is based on data collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1. The observed significance of the signal is 4.9 standard deviations, where a significance of 4.6 standard deviations is expected in the standard model predictions. The results are combined with previously published CMS results based on sqrt(s)=8 TeV data, which leads to an observed (expected) significance of 5.3 (4.8) standard deviations. The measured value of the fiducial cross section for the signal is reported. Bounds are given on quartic vector boson interactions in the framework of dimension-8 effective field theory operators at 95% confidence level.
DOI: 10.17182/hepdata.95244.v1/t1
title: "Table 1" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured second cumulants of net-proton distributions.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t2
title: "Table 2" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Second cumulants of the Skellam distribution.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t3
title: "Table 3" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured second cumulants of protons.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t4
title: "Table 4" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured second cumulants of anti-protons.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t5
title: "Table 5" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured first cumulants of protons.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t6
title: "Table 6" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured first cumulants of anti-protons.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.
DOI: 10.17182/hepdata.95244.v1/t7
title: "Table 7" of "Global baryon number conservation encoded in net-proton fluctuations measured in Pb–Pb collisions at sNN=2.76 TeV"

description: Measured R1 values.
description: CERN-LHC. Experimental results are presented on event-by-event net-proton fluctuation measurements in Pb--Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76$~TeV, recorded by the ALICE detector at the CERN LHC. These measurements have as their ultimate goal an experimental test of Lattice QCD (LQCD) predictions on second and higher order cumulants of net-baryon distributions to search for critical behavior near the QCD phase boundary. Before confronting them with LQCD predictions, account has to be taken of correlations stemming from baryon number conservation as well as fluctuations of participating nucleons. Both effects influence the experimental measurements and are usually not considered in theoretical calculations. For the first time, it is shown that event-by-event baryon number conservation leads to subtle long-range correlations arising from very early interactions in the collisions.