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CMS-SMP-22-006 ; CERN-EP-2023-203
Observation of WW$\gamma $ production and search for H$ \gamma $ production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV
Phys. Rev. Lett. 132 (2024) 121901
Abstract: The observation of WW$\gamma $ production in proton-proton collisions at a center-of-mass energy of 13 TeV with an integrated luminosity of 138 fb$ ^{-1} $ is presented. The observed (expected) significance is 5.6 (4.7) standard deviations. Events are selected by requiring exactly two leptons (one electron and one muon) of opposite charge, moderate missing transverse momentum, and a photon. The measured fiducial cross section for WW$\gamma $ is 6.0 $ \pm $ 0.8 (stat) $ \pm $ 0.7 (syst) $ \pm $ 0.6 (modeling) fb, in agreement with the next-to-leading order quantum chromodynamics prediction. The analysis is extended with a search for the associated production of the Higgs boson and a photon, which is generated by a coupling of the Higgs boson to light quarks. The result is used to constrain the Higgs boson couplings to light quarks.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Representative Feynman diagrams for the WW$\gamma $ process at LO, from left to right: ISR, TGC, QGC, and H$ \gamma $ associated production.

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Figure 1-a:
Representative Feynman diagrams for the WW$\gamma $ process at LO, from left to right: ISR, TGC, QGC, and H$ \gamma $ associated production.

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Figure 1-b:
Representative Feynman diagrams for the WW$\gamma $ process at LO, from left to right: ISR, TGC, QGC, and H$ \gamma $ associated production.

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Figure 1-c:
Representative Feynman diagrams for the WW$\gamma $ process at LO, from left to right: ISR, TGC, QGC, and H$ \gamma $ associated production.

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Figure 1-d:
Representative Feynman diagrams for the WW$\gamma $ process at LO, from left to right: ISR, TGC, QGC, and H$ \gamma $ associated production.

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Figure 2:
The distributions of the invariant mass of the dilepton-photon system (left) and the transverse mass of the WW system (right) after the signal region selection before the fit to the data. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the Monte Carlo statistical uncertainties.

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Figure 2-a:
The distribution of the invariant mass of the dilepton-photon system after the signal region selection before the fit to the data. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the Monte Carlo statistical uncertainties.

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Figure 2-b:
The distribution of the transverse mass of the WW system after the signal region selection before the fit to the data. The black points with error bars represent the data and their statistical uncertainties, whereas the shaded band represents the Monte Carlo statistical uncertainties.

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Figure 3:
The unrolled two-dimensional $ m_{\mathrm{T}}^{\mathrm{W}\mathrm{W}} $ - $ m_{\ell\ell\gamma} $ distributions in category 0 jet (left) and $ \geq $1 jet (right) after the fit to data. The data are compared with the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.

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Figure 3-a:
The unrolled two-dimensional $ m_{\mathrm{T}}^{\mathrm{W}\mathrm{W}} $ - $ m_{\ell\ell\gamma} $ distribution in category 0 jet after the fit to data. The data are compared with the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.

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Figure 3-b:
The unrolled two-dimensional $ m_{\mathrm{T}}^{\mathrm{W}\mathrm{W}} $ - $ m_{\ell\ell\gamma} $ distribution in category $ \geq $1 jet after the fit to data. The data are compared with the sum of the signal and expected background. The black points with error bars represent the data and their statistical uncertainties, whereas the hatched bands represent the total uncertainties in the predictions.
Tables

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Table 1:
The number of events in data and prediction after the fit to data in the SR, SSWW$\gamma $ CR and Top$ \gamma $ CR. The uncertainties include both statistical and systematic contributions.

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Table 2:
Upper limits on the cross section and derived limits in terms of Yukawa coupling at 95% CL for H$ \gamma $ production initiated by light quarks.
Summary
In summary, this letter reports the first observation of WW$\gamma $ production in proton-proton collisions. The measurement uses a data set collected by the CMS experiment at the LHC in 2016--2018 at a center-of-mass energy of 13 TeV, with an integrated luminosity of 138 fb$ ^{-1} $. The measured fiducial cross section for WW$\gamma $ production is 6.0 $ \pm $ 1.2 fb, in agreement with the prediction at next-to-leading order in quantum chromodynamics. A search for the associated production of the Higgs boson and a photon is also performed using the Higgs boson decay to W$^{+}$W$^{-}$. A set of limits at 95% confidence level on the Higgs boson couplings to light quarks is reported.
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