cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127991.v1/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: 10.25549/vercoutere-ouc113056899
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.v1/t26
title: "Figure 9d" 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, 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.v1/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.
DOI: 10.17182/hepdata.127991.v1/t28
title: "Figure 11" 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: The 68 and 95% CL intervals in the likelihood fit with the ttW+ and ttW− cross sections measured independently.
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.v1/t29
title: "Figure 12" 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: Negative log-likelihood value difference with respect to the best fit value for the scan of the ratio between the ttW+ and ttW- cross section.
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/t1
title: "Figure 2a" 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 leading lepton transverse momemtum, 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/t2
title: "Figure 2b" 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 subleading lepton transverse momemtum, 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/t3
title: "Figure 2c" 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 leading jet transverse momemtum, 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/t4
title: "Figure 2d" 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.
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/t5
title: "Figure 2e" 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.
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/t10
title: "Figure 4c" 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 leading jet transverse momemtum, 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/t11
title: "Figure 4d" 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 leading lepton transverse momemtum, 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/t13
title: "Figure 6" 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 and b-tagged jets, prefit, control region enriched in ZZ 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/t6
title: "Figure 2f" 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 missing transverse momemtum, 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/t7
title: "Figure 3" 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 b-tagged jets, 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.