CMS-TOP-23-004 ; CERN-EP-2024-251 | ||
Measurements of inclusive and differential cross sections for top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | ||
CMS Collaboration | ||
30 October 2024 | ||
Submitted to J. High Energy Phys. | ||
Abstract: Measurements are presented of inclusive and differential cross sections for Z boson associated production of top quark pairs ($ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $) and single top quarks ($ \mathrm{t}\mathrm{Z}\mathrm{q} $ or $ \mathrm{t}\mathrm{W}\mathrm{Z} $). The data were recorded in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. Events with three or more leptons, electrons or muons, are selected and a multiclass deep neural network is used to separate three event categories, the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ processes, the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process, and the backgrounds. A profile likelihood approach is used to unfold the differential cross sections, to account for systematic uncertainties, and to determine the correlations between the two signal categories in one global fit. The inclusive cross sections for a dilepton invariant mass between 70 and 110 GeV are measured to be 1.14 $ \pm $ 0.07 pb for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $, and 0.81 $ \pm $ 0.10 pb for $ \mathrm{t}\mathrm{Z}\mathrm{q} $, in good agreement with theoretical predictions. | ||
Links: e-print arXiv:2410.23475 [hep-ex] (PDF) ; CDS record ; inSPIRE record ; HepData record ; CADI line (restricted) ; |
Figures | |
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Figure 1:
Leading order Feynman diagrams for the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ (left), $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (middle), and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (right) processes. |
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Figure 1-a:
Leading order Feynman diagrams for the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ (left), $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (middle), and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (right) processes. |
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Figure 1-b:
Leading order Feynman diagrams for the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ (left), $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (middle), and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (right) processes. |
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Figure 1-c:
Leading order Feynman diagrams for the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ (left), $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (middle), and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (right) processes. |
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Figure 2:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 2-a:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 2-b:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 2-c:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 2-d:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 2-e:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (middle left), the number of b jets (middle right), and the $ |\eta| $ of the jet with the highest $ |\eta| $ (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3-a:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3-b:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3-c:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3-d:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 3-e:
Distributions after final event selection: the $ p_{\mathrm{T}} $ of the reconstructed Z boson (upper left), the $ p_{\mathrm{T}} $ of the lepton arising from the W boson $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and the cosine of the angle $ \cos\theta^\ast_{\mathrm{Z}} $ between the Z boson and its negatively charged decay lepton in the Z boson rest frame (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 4:
Distributions for events selected in the region with $ |m({{\ell}^{+}} {{\ell}^{-}} )-m(\mathrm{Z})| > $ 20 GeV for: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (lower left), and the number of b jets (lower right). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 4-a:
Distributions for events selected in the region with $ |m({{\ell}^{+}} {{\ell}^{-}} )-m(\mathrm{Z})| > $ 20 GeV for: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (lower left), and the number of b jets (lower right). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 4-b:
Distributions for events selected in the region with $ |m({{\ell}^{+}} {{\ell}^{-}} )-m(\mathrm{Z})| > $ 20 GeV for: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (lower left), and the number of b jets (lower right). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 4-c:
Distributions for events selected in the region with $ |m({{\ell}^{+}} {{\ell}^{-}} )-m(\mathrm{Z})| > $ 20 GeV for: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (lower left), and the number of b jets (lower right). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 4-d:
Distributions for events selected in the region with $ |m({{\ell}^{+}} {{\ell}^{-}} )-m(\mathrm{Z})| > $ 20 GeV for: the $ p_{\mathrm{T}} $ of the lepton with the highest (upper left) and second highest (upper right) $ p_{\mathrm{T}} $, the number of jets (lower left), and the number of b jets (lower right). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-a:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-b:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-c:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-d:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-e:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 5-f:
Distributions of the output values in the three DNN output nodes for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ (upper), $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle), and background (lower). The data are compared with expectations. In the left column, the inclusive distributions are shown, i.e.,, each selected event enters each of the output nodes. In the right column, each event enters exactly one of the three distributions, namely the one for which the output score is largest. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 6:
Distributions of the b jet multiplicity in the four lepton region (left) and the jet multiplicity in the zero b jet control region (right). The data are compared to the expectation. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 6-a:
Distributions of the b jet multiplicity in the four lepton region (left) and the jet multiplicity in the zero b jet control region (right). The data are compared to the expectation. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 6-b:
Distributions of the b jet multiplicity in the four lepton region (left) and the jet multiplicity in the zero b jet control region (right). The data are compared to the expectation. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7-a:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7-b:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7-c:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7-d:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 7-e:
Postfit distributions of the b jet multiplicity in events with four leptons (upper left) and the jet multiplicity distribution in events with zero b jets (upper right). Postfit distributions in the output nodes for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ (middle left), $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ (middle right), and the background (lower). The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 8:
Profile likelihood ratio of the two measured inclusive cross sections normalized to the SM predictions $ \mu_{{\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z}} $ and $ \mu_{\mathrm{t}\mathrm{Z}\mathrm{q}} $. The color axis shows twice the negative log-likelihood difference. The measurement is indicated by a cross, and the SM prediction by a diamond. The 68% and 95% confidence levels (CL) ($ -2\Delta\ln{L}= $ 2.30 and 5.99, respectively) are indicated by the red lines. |
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Figure 9:
Prefit (upper) and postfit (lower) output node distributions for the sum of the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ processes. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 10. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 9-a:
Prefit (upper) and postfit (lower) output node distributions for the sum of the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ processes. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 10. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 9-b:
Prefit (upper) and postfit (lower) output node distributions for the sum of the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ processes. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 10. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 10:
Prefit (upper) and postfit (lower) output node distributions for the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 9. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 10-a:
Prefit (upper) and postfit (lower) output node distributions for the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 9. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 10-b:
Prefit (upper) and postfit (lower) output node distributions for the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process. Separate templates are shown for each bin of reconstructed $ p_{\mathrm{T}}(\mathrm{Z}) $. The signal samples are further split into four components each, shown by different colors, according to the generator-level bins of $ p_{\mathrm{T}}(\mathrm{Z}) $. The fit is performed simultaneously on this distribution and that in Fig. 9. The data are displayed as points with statistical error bars and the expectation is shown with a histogram with the systematic uncertainty given by the hatched area. |
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Figure 11:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-a:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-b:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-c:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-d:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-e:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 11-f:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
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Figure 12:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 12-a:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 12-b:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 12-c:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 12-d:
Differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-a:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-b:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-c:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-d:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-e:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 13-f:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $ (upper), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (middle), and $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 14:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 14-a:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 14-b:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 14-c:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 14-d:
Normalized differential cross sections for the sum of $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ production (left column) and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production (right column) as a function of $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (upper), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The inner (outer) error bars indicate the statistical (total) uncertainty, while the shaded area refers to the uncertainty in the theory prediction. The lower panel shows the ratio of the prediction with the data. The points at unity show the uncertainty of the data. |
png pdf |
Figure 15:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
png pdf |
Figure 15-a:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
png pdf |
Figure 15-b:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
png pdf |
Figure 15-c:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
png pdf |
Figure 15-d:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
png pdf |
Figure 15-e:
Covariance matrices for the simultaneous measurement of the differential cross section as a function of $ p_{\mathrm{T}}(\mathrm{Z}) $, (upper left), $ p_{\mathrm{T}}({{\ell}{\mathrm{W}}} ) $ (upper right), $ \Delta R(\mathrm{Z},{{\ell}{\mathrm{W}}} ) $ (middle left), $ \Delta\phi({{\ell}^{+}},{{\ell}^{-}} ) $ (middle right), and $ \cos\theta^\ast_{\mathrm{Z}} $ (lower). The last digits in the axis labels refer to the respective bin of the corresponding differential cross section measurement. |
Tables | |
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Table 1:
Systematic uncertainty sources and their relative impact on the inclusive $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ and $ \mathrm{t}\mathrm{Z}\mathrm{q} $ cross section measurements. |
Summary |
A first simultaneous measurement of single and pair production of top quarks in association with a Z boson is presented. The data were recorded by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. Events with three or more leptons (electrons or muons) are analysed. The separation between the signals is achieved using a deep neural network classifier with three output nodes for the combined $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ and $ \mathrm{t}\mathrm{W}\mathrm{Z} $ processes, the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process, and the backgrounds. The inclusive cross sections are measured to be $ \sigma({\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z})= $ 1.14 $ \pm $ 0.07 pb for the sum of the $ \mathrm{t}\mathrm{W}\mathrm{Z} $ and $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ processes, and $ \sigma(\mathrm{t}\mathrm{Z}\mathrm{q})= $ 0.81 $ \pm $ 0.10 pb for $ \mathrm{t}\mathrm{Z}\mathrm{q} $ production. Both results are evaluated for a dilepton invariant mass between 70 and 110 GeV. The cross sections are measured differentially as functions of several observables. Good agreement with theoretical predictions is found for the $ \mathrm{t}\mathrm{Z}\mathrm{q} $ process, while for $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}\text{+}\mathrm{t}\mathrm{W}\mathrm{Z} $ production, the slope in the transverse momentum distribution of the lepton that originates from the W boson is found to be somewhat steeper than predicted. |
References | ||||
1 | R. Röntsch and M. Schulze | Constraining couplings of top quarks to the Z boson in $ \mathrm{t} \overline{\mathrm{t}} $ +Z production at the LHC | JHEP 07 (2014) 091 | 1404.1005 |
2 | LHC Higgs Cross Section Working Group, D. de Florian et al. | Handbook of LHC Higgs cross sections: 4. Deciphering the nature of the Higgs sector | CERN Report CERN-2017-002-M, 2016 link |
1610.07922 |
3 | ATLAS Collaboration | Measurement of the $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{W}} $ and $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}} $ production cross sections in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 8 TeV with the ATLAS detector | JHEP 11 (2015) 172 | 1509.05276 |
4 | ATLAS Collaboration | Measurement of the $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}} $ and $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{W}} $ production cross sections in multilepton final states using 3.2 fb$ ^{-1} $ of $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector | EPJC 77 (2017) 40 | 1609.01599 |
5 | ATLAS Collaboration | Measurement of the production cross-section of a single top quark in association with a Z boson in proton-proton collisions at 13 TeV with the ATLAS detector | PLB 780 (2018) 557 | 1710.03659 |
6 | ATLAS Collaboration | Measurement of the $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}} $ and $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{W}} $ cross sections in proton-proton collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector | PRD 99 (2019) 072009 | 1901.03584 |
7 | ATLAS Collaboration | Observation of the associated production of a top quark and a Z boson in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector | JHEP 07 (2020) 124 | 2002.07546 |
8 | ATLAS Collaboration | Measurements of the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a Z boson at $ \sqrt{s}= $ 13 TeV with the ATLAS detector | EPJC 81 (2021) 737 | 2103.12603 |
9 | ATLAS Collaboration | Inclusive and differential cross-section measurements of $ {{\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z}} $ production in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector, including EFT and spin-correlation interpretations | JHEP 07 (2024) 163 | 2312.04450 |
10 | CMS Collaboration | Observation of top quark pairs produced in association with a vector boson in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 8 TeV | JHEP 01 (2016) 096 | CMS-TOP-14-021 1510.01131 |
11 | CMS Collaboration | Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JHEP 08 (2018) 011 | CMS-TOP-17-005 1711.02547 |
12 | CMS Collaboration | Measurement of the associated production of a single top quark and a Z boson in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV | PLB 779 (2018) 358 | CMS-TOP-16-020 1712.02825 |
13 | CMS Collaboration | Observation of single top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | PRL 122 (2019) 132003 | CMS-TOP-18-008 1812.05900 |
14 | CMS Collaboration | Measurement of top quark pair production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JHEP 03 (2020) 056 | CMS-TOP-18-009 1907.11270 |
15 | CMS Collaboration | Inclusive and differential cross section measurements of single top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JHEP 02 (2022) 107 | CMS-TOP-20-010 2111.02860 |
16 | J. Campbell, R. K. Ellis, and R. Röntsch | Single top production in association with a Z boson at the LHC | PRD 87 (2013) 114006 | 1302.3856 |
17 | S. Frixione et al. | Electroweak and QCD corrections to top-pair hadroproduction in association with heavy bosons | JHEP 06 (2015) 184 | 1504.03446 |
18 | R. Frederix et al. | The automation of next-to-leading order electroweak calculations | JHEP 07 (2018) 185 | 1804.10017 |
19 | A. Kulesza et al. | Associated top-pair production with a heavy boson production through NLO+NNLL accuracy at the LHC | in Proc. 54th Rencontres de Moriond on QCD and High Energy Interactions (Moriond QCD ): La Thuile, Italy, 2019 | 1905.07815 |
20 | D. Pagani, I. Tsinikos, and E. Vryonidou | NLO QCD+EW predictions for $ {\mathrm{t}\mathrm{H}\mathrm{j}} $ and $ {\mathrm{t}\mathrm{Z}\mathrm{j}} $ production at the LHC | JHEP 08 (2020) 082 | 2006.10086 |
21 | CMS Collaboration | Evidence for $ {\mathrm{t}\mathrm{W}\mathrm{Z}} $ production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV in multilepton final states | PLB 855 (2024) 138815 | CMS-TOP-22-008 2312.11668 |
22 | J. Alwall et al. | The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations | JHEP 07 (2014) 079 | 1405.0301 |
23 | H. El Faham, F. Maltoni, K. Mimasu, and M. Zaro | Single top production in association with a $ {\mathrm{W}\mathrm{Z}} $ pair at the LHC in the SMEFT | JHEP 01 (2022) 100 | 2111.03080 |
24 | W. Buchmuller and D. Wyler | Effective Lagrangian analysis of new interactions and flavour conservation | NPB 268 (1986) 621 | |
25 | C. P. Burgess | An introduction to effective field theory | Ann. Rev. Nucl. Part. Sci. 57 (2007) 329 | hep-th/0701053 |
26 | SMEFiT Collaboration | Combined SMEFT interpretation of Higgs, diboson, and top quark data from the LHC | JHEP 11 (2021) 089 | 2105.00006 |
27 | N. Castro et al. | LHC EFT WG report: Experimental measurements and observables | LHC EFT Working Group Public Note CERN-LHCEFTWG-2022-001, 2022 | 2211.08353 |
28 | CMS Collaboration | HEPData record for this analysis | link | |
29 | CMS Collaboration | The CMS experiment at the CERN LHC | JINST 3 (2008) S08004 | |
30 | CMS Collaboration | Development of the CMS detector for the CERN LHC \mboxRun 3 | JINST 19 (2024) P05064 | CMS-PRF-21-001 2309.05466 |
31 | CMS Collaboration | Particle-flow reconstruction and global event description with the CMS detector | JINST 12 (2017) P10003 | CMS-PRF-14-001 1706.04965 |
32 | CMS Collaboration | Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid | CMS Technical Proposal CERN-LHCC-2015-010, CMS-TDR-15-02, 2015 link |
|
33 | M. Cacciari, G. P. Salam, and G. Soyez | The anti-$ k_{\mathrm{T}} $ jet clustering algorithm | JHEP 04 (2008) 063 | 0802.1189 |
34 | M. Cacciari, G. P. Salam, and G. Soyez | FASTJET user manual | EPJC 72 (2012) 1896 | 1111.6097 |
35 | CMS Collaboration | Pileup mitigation at CMS in 13 TeV data | JINST 15 (2020) P09018 | CMS-JME-18-001 2003.00503 |
36 | CMS Collaboration | Jet energy scale and resolution in the CMS experiment in $ {\mathrm{p}\mathrm{p}} $ collisions at 8 TeV | JINST 12 (2017) P02014 | CMS-JME-13-004 1607.03663 |
37 | CMS Collaboration | Identification of heavy-flavour jets with the CMS detector in $ {\mathrm{p}\mathrm{p}} $ collisions at 13 TeV | JINST 13 (2018) P05011 | CMS-BTV-16-002 1712.07158 |
38 | CMS Collaboration | Performance of missing transverse momentum reconstruction in proton-proton collisions at $ \sqrt{s}= $ 13 TeV using the CMS detector | JINST 14 (2019) P07004 | CMS-JME-17-001 1903.06078 |
39 | S. Frixione, P. Nason, and C. Oleari | Matching NLO QCD computations with parton shower simulations: the POWHEG method | JHEP 11 (2007) 070 | 0709.2092 |
40 | J. M. Campbell and R. K. Ellis | MCFM for the Tevatron and the LHC | in Proc. 10th DESY Workshop on Elementary Particle Theory: Loops and Legs in Quantum Field Theory (LL): Wörlitz, Germany, 2010 Nucl. Phys. B Proc. Suppl. 205 10 |
1007.3492 |
41 | T. Sjöstrand et al. | An introduction to PYTHIA8.2 | Comput. Phys. Commun. 191 (2015) 159 | 1410.3012 |
42 | CMS Collaboration | Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements | EPJC 80 (2020) 4 | CMS-GEN-17-001 1903.12179 |
43 | R. Frederix and S. Frixione | Merging meets matching in MC@NLO | JHEP 12 (2012) 061 | 1209.6215 |
44 | J. Alwall et al. | Comparative study of various algorithms for the merging of parton showers and matrix elements in hadronic collisions | EPJC 53 (2008) 473 | 0706.2569 |
45 | NNPDF Collaboration | Parton distributions from high-precision collider data | EPJC 77 (2017) 663 | 1706.00428 |
46 | S. Frixione et al. | Single-top hadroproduction in association with a W boson | JHEP 07 (2008) 029 | 0805.3067 |
47 | F. Demartin et al. | $ {\mathrm{t}\mathrm{W}\mathrm{H}} $ associated production at the LHC | EPJC 77 (2017) 34 | 1607.05862 |
48 | GEANT4 Collaboration | GEANT 4---a simulation toolkit | NIM A 506 (2003) 250 | |
49 | CMS Collaboration | Observation of four top quark production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | PLB 847 (2023) 138290 | CMS-TOP-22-013 2305.13439 |
50 | CMS Collaboration | Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC | JINST 16 (2021) P05014 | CMS-EGM-17-001 2012.06888 |
51 | CMS Collaboration | Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JINST 13 (2018) P06015 | CMS-MUO-16-001 1804.04528 |
52 | M. Abadi et al. | TensorFlow: Large-scale machine learning on heterogeneous systems | link | |
53 | F. Chollet et al. | keras | link | |
54 | Particle Data Group , R. L. Workman et al. | Review of particle physics | Prog. Theor. Exp. Phys. 2022 (2022) 083C01 | |
55 | CMS Collaboration | Performance of the CMS muon trigger system in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JINST 16 (2021) P07001 | CMS-MUO-19-001 2102.04790 |
56 | CMS Collaboration | Performance of the CMS Level-1 trigger in proton-proton collisions at $ \sqrt{s}= $ 13 TeV | JINST 15 (2020) P10017 | CMS-TRG-17-001 2006.10165 |
57 | CMS Collaboration | Measurement of the inelastic proton-proton cross section at $ \sqrt{s}= $ 13 TeV | JHEP 07 (2018) 161 | CMS-FSQ-15-005 1802.02613 |
58 | CMS Collaboration | Precision luminosity measurement in proton-proton collisions at $ \sqrt{s}= $ 13 TeV in 2015 and 2016 at CMS | EPJC 81 (2021) 800 | CMS-LUM-17-003 2104.01927 |
59 | CMS Collaboration | CMS luminosity measurement for the 2017 data-taking period at $ \sqrt{s}= $ 13 TeV | CMS Physics Analysis Summary, 2018 CMS-PAS-LUM-17-004 |
CMS-PAS-LUM-17-004 |
60 | CMS Collaboration | CMS luminosity measurement for the 2018 data-taking period at $ \sqrt{s}= $ 13 TeV | CMS Physics Analysis Summary, 2019 CMS-PAS-LUM-18-002 |
CMS-PAS-LUM-18-002 |
61 | J. Butterworth et al. | PDF4LHC recommendations for LHC \mboxRun 2 | JPG 43 (2016) 023001 | 1510.03865 |
62 | S. Argyropoulos and T. Sjöstrand | Effects of color reconnection on $ \mathrm{t} \overline{\mathrm{t}} $ final states at the LHC | JHEP 11 (2014) 043 | 1407.6653 |
63 | R. Barlow and C. Beeston | Fitting using finite Monte Carlo samples | Comput. Phys. Commun. 77 (1993) 219 | |
64 | CMS Collaboration | The CMS statistical analysis and combination tool: combine | Accepted by Comput. Softw. Big Sci, 2024 | CMS-CAT-23-001 2404.06614 |
65 | CMS Collaboration | Probing effective field theory operators in the associated production of top quarks with a Z boson in multilepton final states at $ \sqrt{s}= $ 13 TeV | JHEP 12 (2021) 083 | CMS-TOP-21-001 2107.13896 |
66 | C. Degrande et al. | Single-top associated production with a Z or H boson at the LHC: the SMEFT interpretation | JHEP 10 (2018) 005 | 1804.07773 |
67 | D. Spitzbart | Search for supersymmetric partners and anomalous couplings of the top quark with the CMS experiment | PhD thesis, Technische Universität Wien, 2019 link |
|
68 | CMS Collaboration | Differential cross section measurements for the production of top quark pairs and of additional jets using dilepton events from $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV | Submitted to JHEP, 2024 | CMS-TOP-20-006 2402.08486 |
69 | CMS Collaboration | Measurements of $ \mathrm{t} \overline{\mathrm{t}} $ differential cross sections in proton-proton collisions at $ \sqrt{s}= $ 13 TeV using events containing two leptons | JHEP 02 (2019) 149 | CMS-TOP-17-014 1811.06625 |
70 | CMS Collaboration | Measurement of differential cross sections for the production of top quark pairs and of additional jets in lepton+jets events from $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV | PRD 97 (2018) 112003 | CMS-TOP-17-002 1803.08856 |
Compact Muon Solenoid LHC, CERN |