cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127991.v2/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.v2/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/t30
title: "Figure 1 - Supplemental Material" 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, 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/t31
title: "Figure 2 - Supplemental Material" 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, 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-ouc110610862
title: 2 nude women, a mask, and a desk

description: Two females: one green and black nude with red highlights in pubic area and ribs is standing depicted from knees to breasts; the other yellow nude sitting with legs spread depicted from knees to chin; orange mask, against a striped red and green wall and brown desk. See description of 001 for OT notes.
DOI: 10.17182/hepdata.127991.v2/t24
title: "Figure 9b" 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, 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/t32
title: "Figure 3 - Supplemental Material" 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, 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/t33
title: "Figure 4 - Supplemental Material" 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, 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/t34
title: "Figure 5 - Supplemental Material" 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, 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/t35
title: "Figure 6 - Supplemental Material" 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, 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/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.v2/t36
title: "Figure 7 - Supplemental Material" 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, 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.127992.v1/t1
title: "Figure 1 dR" of "Measurement of the $\mathrm{t\bar{t}}$ charge asymmetry in events with highly Lorentz-boosted top quarks in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the distance between the lepton and the closest AK4 jet. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
description: The measurement of the charge asymmetry in top quark pair events with highly Lorentz-boosted top quarks decaying to a single lepton and jets is presented. The analysis is performed using proton-proton collisions at $\sqrt{s}=13\TeV$ with the CMS detector at the LHC and corresponding to an integrated luminosity of 138\fbinv. The selection is optimized for top quarks produced with large Lorentz boosts, resulting in nonisolated leptons and overlapping jets. The top quark charge asymmetry is measured for events with a \ttbar invariant mass larger than $750{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$ and corrected for detector and acceptance effects using a binned maximum likelihood fit. The measured top quark charge asymmetry of $(0.69_{\;- 0.69}^{\;+ 0.65})\%$ is in good agreement with the standard model prediction at next-to-next-to-leading order in quantum chromodynamic perturbation theory with next-to-leading-order electroweak corrections. The result is also presented for two invariant mass ranges, 750--900 and $&gt; 900{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$.
DOI: 10.17182/hepdata.127992.v1/t2
title: "Figure 1 Njets" of "Measurement of the $\mathrm{t\bar{t}}$ charge asymmetry in events with highly Lorentz-boosted top quarks in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the number of AK4 jets. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
description: The measurement of the charge asymmetry in top quark pair events with highly Lorentz-boosted top quarks decaying to a single lepton and jets is presented. The analysis is performed using proton-proton collisions at $\sqrt{s}=13\TeV$ with the CMS detector at the LHC and corresponding to an integrated luminosity of 138\fbinv. The selection is optimized for top quarks produced with large Lorentz boosts, resulting in nonisolated leptons and overlapping jets. The top quark charge asymmetry is measured for events with a \ttbar invariant mass larger than $750{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$ and corrected for detector and acceptance effects using a binned maximum likelihood fit. The measured top quark charge asymmetry of $(0.69_{\;- 0.69}^{\;+ 0.65})\%$ is in good agreement with the standard model prediction at next-to-next-to-leading order in quantum chromodynamic perturbation theory with next-to-leading-order electroweak corrections. The result is also presented for two invariant mass ranges, 750--900 and $&gt; 900{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$.
DOI: 10.17182/hepdata.127992.v1/t3
title: "Figure 1 Mttbar" of "Measurement of the $\mathrm{t\bar{t}}$ charge asymmetry in events with highly Lorentz-boosted top quarks in pp collisions at $\sqrt{s}$ = 13 TeV"

description: Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the reconstruced mass of the top quark pairs. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
description: The measurement of the charge asymmetry in top quark pair events with highly Lorentz-boosted top quarks decaying to a single lepton and jets is presented. The analysis is performed using proton-proton collisions at $\sqrt{s}=13\TeV$ with the CMS detector at the LHC and corresponding to an integrated luminosity of 138\fbinv. The selection is optimized for top quarks produced with large Lorentz boosts, resulting in nonisolated leptons and overlapping jets. The top quark charge asymmetry is measured for events with a \ttbar invariant mass larger than $750{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$ and corrected for detector and acceptance effects using a binned maximum likelihood fit. The measured top quark charge asymmetry of $(0.69_{\;- 0.69}^{\;+ 0.65})\%$ is in good agreement with the standard model prediction at next-to-next-to-leading order in quantum chromodynamic perturbation theory with next-to-leading-order electroweak corrections. The result is also presented for two invariant mass ranges, 750--900 and $&gt; 900{\ensuremath{\,\text{Ge\hspace{-.08em}V}}\xspace}$.