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CMS-HIG-20-013 ; CERN-EP-2022-120
Measurements of the Higgs boson production cross section and couplings in the WW boson pair decay channel in proton-proton collisions at $\sqrt{s} = $ 13 TeV
Eur. Phys. J. C 83 (2023) 667
Abstract: Production cross sections of the standard model Higgs boson decaying to a pair of W bosons are measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analysis targets Higgs bosons produced via gluon fusion, vector boson fusion, and in association with a W or Z boson. Candidate events are required to have at least two charged leptons and moderate missing transverse momentum, targeting events with at least one leptonically decaying W boson originating from the Higgs boson. Results are presented in the form of inclusive and differential cross sections in the simplified template cross section framework, as well as couplings of the Higgs boson to vector bosons and fermions. The data set collected by the CMS detector during 2016-2018 is used, corresponding to an integrated luminosity of 138 fb$^{-1}$. The signal strength modifier $\mu$, defined as the ratio of the observed production rate in a given decay channel to the standard model expectation, is measured to be $\mu = $ 0.95$^{+0.10}_{-0.09}$. All results are found to be compatible with the standard model within the uncertainties.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 0-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. The uncertainty band corresponds to the total systematic uncertainty in the templates after the fit to the data. The signal template is shown both stacked on top of the backgrounds, as well as superimposed. The predicted yields are shown with their best fit normalizations from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The overflow is included in the last bin. The lower panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction.

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Figure 1-a:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 0-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. The uncertainty band corresponds to the total systematic uncertainty in the templates after the fit to the data. The signal template is shown both stacked on top of the backgrounds, as well as superimposed. The predicted yields are shown with their best fit normalizations from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The overflow is included in the last bin. The lower panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction.

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Figure 1-b:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 0-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. The uncertainty band corresponds to the total systematic uncertainty in the templates after the fit to the data. The signal template is shown both stacked on top of the backgrounds, as well as superimposed. The predicted yields are shown with their best fit normalizations from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The overflow is included in the last bin. The lower panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction.

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Figure 1-c:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 0-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. The uncertainty band corresponds to the total systematic uncertainty in the templates after the fit to the data. The signal template is shown both stacked on top of the backgrounds, as well as superimposed. The predicted yields are shown with their best fit normalizations from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The overflow is included in the last bin. The lower panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction.

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Figure 1-d:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 0-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. The uncertainty band corresponds to the total systematic uncertainty in the templates after the fit to the data. The signal template is shown both stacked on top of the backgrounds, as well as superimposed. The predicted yields are shown with their best fit normalizations from the simultaneous fit. Vertical bars on data points represent the statistical uncertainty in the data. The overflow is included in the last bin. The lower panel in each figure shows the ratio of the number of events observed in data to that of the total SM prediction.

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Figure 2:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 1-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. A detailed description is given in the Fig. 1 caption.

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Figure 2-a:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 1-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. A detailed description is given in the Fig. 1 caption.

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Figure 2-b:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 1-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. A detailed description is given in the Fig. 1 caption.

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Figure 2-c:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 1-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. A detailed description is given in the Fig. 1 caption.

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Figure 2-d:
Observed distributions of the ${m_{\ell \ell}}$ (upper) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (lower) fit variables in the 1-jet ggH $ {{p_{\mathrm {T}}} {}_2} < $ 20 GeV (left) and $ {{p_{\mathrm {T}}} {}_2} > $ 20 GeV (right) DF categories. A detailed description is given in the Fig. 1 caption.

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Figure 3:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) fit variables in the 2-jet ggH DF category. A detailed description is given in the Fig. 1 caption.

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Figure 3-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) fit variables in the 2-jet ggH DF category. A detailed description is given in the Fig. 1 caption.

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Figure 3-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) fit variables in the 2-jet ggH DF category. A detailed description is given in the Fig. 1 caption.

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Figure 4:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 4-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 4-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 5:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 5-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 5-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 6:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 6-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 6-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF top quark control region. A detailed description is given in the Fig. 1 caption.

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Figure 7:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 7-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 7-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 0-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 8:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 8-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 8-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 1-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 9:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 9-a:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 9-b:
Observed distributions of the ${m_{\ell \ell}}$ (left) and ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ (right) variables in the 2-jet DF ${\tau \tau}$ control region. A detailed description is given in the Fig. 1 caption.

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Figure 10:
Distributions for the $C_{\mathrm {VBF}}$ (left) and $C_{{\mathrm{g} \mathrm{g} \mathrm{H}}}$ (right) classifiers in the VBF-like and ggH-like VBF DF categories, respectively. A detailed description is given in the Fig. 1 caption.

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Figure 10-a:
Distributions for the $C_{\mathrm {VBF}}$ (left) and $C_{{\mathrm{g} \mathrm{g} \mathrm{H}}}$ (right) classifiers in the VBF-like and ggH-like VBF DF categories, respectively. A detailed description is given in the Fig. 1 caption.

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Figure 10-b:
Distributions for the $C_{\mathrm {VBF}}$ (left) and $C_{{\mathrm{g} \mathrm{g} \mathrm{H}}}$ (right) classifiers in the VBF-like and ggH-like VBF DF categories, respectively. A detailed description is given in the Fig. 1 caption.

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Figure 11:
Distribution of the $C_{\mathrm {VBF}}$ classifier in the VBF DF SR, before the further event categorization based on the classifier outputs. A detailed description is given in the Fig. 1 caption.

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Figure 12:
Observed distributions of the ${\tilde{m}_{\mathrm{H}}}$ fit variable in the WHSS 1-jet e${\mu}$(upper left), 2-jet e${\mu}$(upper right), 1-jet ${\mu}{\mu}$ (lower left), and 2-jet ${\mu}{\mu}$ (lower right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 12-a:
Observed distributions of the ${\tilde{m}_{\mathrm{H}}}$ fit variable in the WHSS 1-jet e${\mu}$(upper left), 2-jet e${\mu}$(upper right), 1-jet ${\mu}{\mu}$ (lower left), and 2-jet ${\mu}{\mu}$ (lower right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 12-b:
Observed distributions of the ${\tilde{m}_{\mathrm{H}}}$ fit variable in the WHSS 1-jet e${\mu}$(upper left), 2-jet e${\mu}$(upper right), 1-jet ${\mu}{\mu}$ (lower left), and 2-jet ${\mu}{\mu}$ (lower right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 12-c:
Observed distributions of the ${\tilde{m}_{\mathrm{H}}}$ fit variable in the WHSS 1-jet e${\mu}$(upper left), 2-jet e${\mu}$(upper right), 1-jet ${\mu}{\mu}$ (lower left), and 2-jet ${\mu}{\mu}$ (lower right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 12-d:
Observed distributions of the ${\tilde{m}_{\mathrm{H}}}$ fit variable in the WHSS 1-jet e${\mu}$(upper left), 2-jet e${\mu}$(upper right), 1-jet ${\mu}{\mu}$ (lower left), and 2-jet ${\mu}{\mu}$ (lower right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 13:
Observed distributions of the BDT score in the WH3$\ell$ OSSF (left) and SSSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 13-a:
Observed distributions of the BDT score in the WH3$\ell$ OSSF (left) and SSSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 13-b:
Observed distributions of the BDT score in the WH3$\ell$ OSSF (left) and SSSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 14:
Observed distributions of the ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ fit variable in the ZH3$\ell$ 1-jet (left) and 2-jet (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 14-a:
Observed distributions of the ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ fit variable in the ZH3$\ell$ 1-jet (left) and 2-jet (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 14-b:
Observed distributions of the ${{m_{\mathrm {T}}} ^{\mathrm{H}}}$ fit variable in the ZH3$\ell$ 1-jet (left) and 2-jet (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 15:
Observed distributions of the BDT score in the ZH4$\ell$ XDF (left) and XSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 15-a:
Observed distributions of the BDT score in the ZH4$\ell$ XDF (left) and XSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 15-b:
Observed distributions of the BDT score in the ZH4$\ell$ XDF (left) and XSF (right) SRs. A detailed description is given in the Fig. 1 caption.

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Figure 16:
Observed distribution of the ${m_{\ell \ell}}$ fit variable in the VH2j DF SR. A detailed description is given in the Fig. 1 caption.

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Figure 17:
The STXS Stage 1.2 binning scheme. Bins fused together with solid colors are measured as a single bin.

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Figure 17-a:
The STXS Stage 1.2 binning scheme. Bins fused together with solid colors are measured as a single bin.

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Figure 17-b:
The STXS Stage 1.2 binning scheme. Bins fused together with solid colors are measured as a single bin.

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Figure 17-c:
The STXS Stage 1.2 binning scheme. Bins fused together with solid colors are measured as a single bin.

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Figure 18:
Analysis categories targeting the STXS bins. The baseline ggH, VBF, and VH selections are identical to what was described in Sections 5-7. All dimensional quantities are measured in GeV.

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Figure 19:
Expected signal composition in each STXS bin. Generator-level bins are reported in the horizontal axis, and the corresponding analysis categories on the vertical axis. All quantities in the definitions of bins are measured in GeV.

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Figure 20:
Expected relative fractions of different STXS signal processes in each category. The total number of expected ${\mathrm{H} \to \mathrm{W} \mathrm{W}}$ signal events in each category is also shown. All dimensional quantities in the definitions of bins are measured in GeV.

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Figure 21:
Distribution of events as a function of the statistical significance of their corresponding bin in the analysis template, including all categories. Signal and background contributions are shown after the fit to the data.

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Figure 22:
Observed profile-likelihood function for the global signal strength modifier $\mu $. The dashed curve corresponds to the profile-likelihood function obtained considering statistical uncertainties only.

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Figure 23:
Observed signal strength modifiers for the main SM production modes.

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Figure 24:
Correlation matrix between the signal strength modifiers of the main production modes of the Higgs boson.

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Figure 25:
Two-dimensional likelihood profile as a function of the coupling modifiers $\kappa _{{\mathrm{V}}}$ and $\kappa _\mathrm {f}$, using the $\kappa $-framework parametrization. The 95 and 68% confidence level contours are shown as continuous and dashed lines, respectively.

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Figure 26:
Observed cross sections in each STXS bin, normalized to the SM expectation.

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Figure 27:
Correlation matrix between the measured STXS bins. All dimensional quantities in bin definitions are measured in GeV.
Tables

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Table 1:
Trigger requirements on the data set used in the analysis.

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Table 2:
Overview of the selection defining the analysis categories (a more detailed breakdown is given in Table 12).

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Table 3:
Summary of the selection used in different-flavor ggH categories.

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Table 4:
Summary of the selection used in same-flavor ggH categories. The DYMVA threshold is optimized separately in each subcategory and data set.

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Table 5:
Selection used in the different-flavor VBF categories.

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Table 6:
Selection used in the same-flavor VBF categories. The DYMVA threshold is optimized separately in each subcategory and data set.

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Table 7:
Event selection and categorization in the WHSS category.

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Table 8:
Event selection and categorization in the WH3$\ell$ category.

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Table 9:
Event selection and categorization in the ZH3$\ell$ category.

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Table 10:
Event selection and categorization in the ZH4$\ell$ category.

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Table 11:
Summary of the selection applied to different-flavor VH2j categories.

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Table 12:
Overview of the fit variables and CRs used in each analysis category. In all CRs, the number of events is used.

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Table 13:
Contributions of different sources of uncertainty in the signal strength measurement. The systematic component includes the combined effect from all sources besides background normalization and the size of the dataset, which make up the statistical part.

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Table 14:
Number of events by process in the ggH DF categories after the fit to the data, scaling the ggH, VBF, WH, and ZH production modes separately. The ${\mathrm{t} {}\mathrm{\bar{t}}}$H contribution is fixed to its SM expectation. Numbers in parenthesis indicate expected yields.

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Table 15:
Number of events by process in the ggH SF categories after the fit to the data, scaling the ggH, VBF, WH, and ZH production modes separately. The ${\mathrm{t} {}\mathrm{\bar{t}}}$H contribution is fixed to its SM expectation. Numbers in parenthesis indicate expected yields.

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Table 16:
Number of events by process in the VBF and VH2j categories after the fit to the data, scaling the ggH, VBF, WH, and ZH production modes separately. The ${\mathrm{t} {}\mathrm{\bar{t}}}$H contribution is fixed to its SM expectation. Numbers in parenthesis indicate expected yields.

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Table 17:
Number of events by process in the ZH4$\ell$, WH3$\ell$, ZH3$\ell$, and ZH4$\ell$ categories after the fit to the data, scaling the ggH, VBF, WH, and ZH production modes separately. The ${\mathrm{t} {}\mathrm{\bar{t}}}$H contribution is fixed to its SM expectation. Numbers in parenthesis indicate expected yields.

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Table 18:
Observed cross sections in each STXS bin. The uncertainties in the observed cross sections and their ratio to the SM expectation do not include the theoretical uncertainties on the latter. In cases where the ratio to the SM cross section is measured below zero, an upper limit at 68% confidence level on the observed cross section is reported. All dimensional quantities in STXS bin definitions are measured in GeV.
Summary
A measurement of production cross sections for the Higgs boson has been performed targeting the gluon fusion, vector boson fusion, and Z or W associated production processes in the ${\mathrm{H}\to\mathrm{W}\mathrm{W}}$ decay channel. Results are presented as signal strength modifiers, coupling modifiers, and differential cross sections in the simplified template cross section Stage 1.2 framework. The measurement has been performed on data from proton-proton collisions recorded by the CMS detector at a center-of-mass energy of 13 TeV in 2016-2018, corresponding to an integrated luminosity of 138 fb$^{-1}$. Specific event selections targeting different final states have been employed, and results have been extracted via a simultaneous maximum likelihood fit to all analysis categories. The overall signal strength for production of a Higgs boson is found to be $\mu = $ 0.95$^{+0.10}_{-0.09}$. All results are in good agreement with the standard model expectation.
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