cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.127990.v1/t4
title: "parton_abs_rho_covariance_extrapolation" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for the extrapolation uncertainty for the measurement of the absolute differential cross section as a function of the rho observable at parton level.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t6
title: "parton_norm_rho_covariance_total" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for the total uncertainty for the measurement of the normalized differential cross section as a function of the rho observable at parton level.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t10
title: "np_impacts_pulls" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: This table is a numerical representation of Fig. 8 for all nuisance parameters.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t5
title: "parton_norm_rho" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Normalized differential cross section as a function of the rho observable at parton level.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t7
title: "parton_norm_rho_covariance_stat" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for the statistical uncertainty for the measurement of the normalized differential cross section as a function of the rho observable at parton level.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t8
title: "parton_norm_rho_covariance_extrapolation" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Covariance matrix for the extrapolation uncertainty for the measurement of the normalized differential cross section as a function of the rho observable at parton level.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127990.v1/t9
title: "fit_np_correlation" of "Measurement of the top quark pole mass using $\mathrm{t\bar{t}}$+jet events in the dilepton final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix for all nuisance parameters and parameters of interest of the Likelihood fit.
description: Measurement of the top quark pole mass using $\text{t}\overline{\text{t}}\text{+jet}$ events in the dilepton final state in proton-proton collisions at$\sqrt{s}=$ 13 TeV. A measurement of the top quark pole mass $m_{\text{t}}^{\text{pole}}$ in events where a top quark-antiquark pair ($\text{t}\overline{\text{t}}$) is produced in association with at least one additional jet ($\text{t}\overline{\text{t}}$+jet) is presented. This analysis is performed using proton-proton collision data at $\sqrt{s}=$ 13 TeV collected by the CMS experiment at the CERN LHC, corresponding to a total integrated luminosity of 36.3fb$^{-1}$. Events with two opposite-sign leptons in the final state ($\text{e}^{+}\text{e}^{-}$, $\mu^{+}\mu^{-}$, $\text{e}^{\pm}\mu^{\mp}$) are analyzed. The reconstruction of the main observable and the event selection are optimized using multivariate analysis techniques based on machine learning. The production cross section is measured as a function of the inverse of the invariant mass of the $\text{t}\overline{\text{t}}$+jet system at the parton level using a maximum likelihood unfolding. Given a reference parton distribution function (PDF), the top quark pole mass is extracted using the theoretical predictions at next-to-leading order. For the ABMP16NLO PDF, this results in $m_{\text{t}}^{\text{pole}}=172.94\pm1.37$.
DOI: 10.17182/hepdata.127991.v1/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.v1/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.v1/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.v1/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.v1/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.v1/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.v1/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.
DOI: 10.25549/vercoutere-ouc113056901
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)