cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127991.v2/t9
title: "Figure 4b" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of the number of loose b-tagged jets, prefit, validation region.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.25549/vercoutere-ouc113056745
title: Publisher correspondence

description: Correspondence between Al Vercoutere and various publishers related to publication of patient artwork in textbooks. Arranged in chronological order includes letters and forms (101), check receipts (9), and envelopes (15)
DOI: 10.17182/hepdata.127991.v2/t12
title: "Figure 5" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of the number of jets based on the number of b-tagged jets, prefit, control region enriched in WZ and ttZ.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t14
title: "Table 1" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Number of predicted and observed events in the signal regions of the dilepton and trilepton channels. The last column shows the ratio between the number of predicted events obtained after and before the fit is performed. The total uncertainty in the number of predicted events is shown. The symbol “—” indicates that the corresponding background does not apply.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t15
title: "Figure 7a" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of NN discriminant with two leptons positive charges, prefit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t18
title: "Figure 7d" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of NN discriminant with two leptons negative charges, postfit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t8
title: "Figure 4a" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of the number of jets, prefit, validation region.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t16
title: "Figure 7b" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of NN discriminant with two leptons negative charges, prefit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t17
title: "Figure 7c" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of NN discriminant with two leptons positive charges, postfit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t19
title: "Figure 8a" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 2 b-tagged jets, positive sum of lepton charges, prefit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t20
title: "Figure 8b" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 3 jets of which exactly 2 are b-tagged jets, positive sum of lepton charges, prefit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t22
title: "Figure 8d" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 3 jets of which exactly 2 are b-tagged jets, positive sum of lepton charges, postfit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t23
title: "Figure 9a" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 2 b-tagged jets, negative sum of lepton charges, prefit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t25
title: "Figure 9c" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 2 b-tagged jets, negative sum of lepton charges, postfit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t21
title: "Figure 8c" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distribution of three-lepton invariant mass with 2 b-tagged jets, positive sum of lepton charges, postfit.
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.
DOI: 10.17182/hepdata.127991.v2/t27
title: "Figure 10" of "Measurement of the cross section of top quark-antiquark pair production in association with a W boson in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Measured cross sections
description: The production of a top quark-antiquark pair in association with a W boson is measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analyzed data was recorded by the CMS experiment at the CERN LHC and corresponds to an integrated luminosity of 138 fb$^{-1}$. Events with two or three leptons (electrons and muons) and additional jets are selected. In events with two leptons, a multiclass neural network is used to distinguish between the signal and background processes. Events with three leptons are categorized based on the number of jets and of jets originating from b quark hadronization, and the lepton charges. The inclusive $t\bar{t}$W production cross section in the full phase space is measured to be 868 $\pm$ 40(stat) $\pm$ 50(syst) fb. The $t\bar{t}$W$^+$ and $t\bar{t}$W$^-$ cross sections are also measured as 553 $\pm$ 30(stat) $\pm$ 30(syst) fb and 343 $\pm$ 26(stat) $\pm$ 25(syst) fb, respectively, and the corresponding ratio of the two cross sections is found to be 1.61 $\pm$ 0.15(stat) $^{+0.07}_{-0.05}$(syst). The results are consistent with the standard model predictions within two standard deviations, and represent the most precise measurement of these cross sections to date.