CMS-PAS-SMP-19-002 | ||
Measurement of the inclusive Wγ production cross section in proton-proton collisions at √s= 13 TeV and constraints on effective field theory coefficients | ||
CMS Collaboration | ||
November 2020 | ||
Abstract: The cross section of inclusive Wγ production in proton-proton collisions at a center-of-mass energy of 13 TeV has been measured based on 137.1 fb−1 of data collected using the CMS experiment at the LHC. Both the electron and the muon decay modes of the W boson are considered by performing a maximum likelihood fit to the lepton-photon mass distribution. The measured cross section is compared to theoretical predictions made at next-to-leading order in quantum chromodynamics. In addition, 95% confidence level limits on anomalous triple gauge couplings are reported within the framework of effective field theory. | ||
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These preliminary results are superseded in this paper, Accepted by PRL. The superseded preliminary plots can be found here. |
Figures | |
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Figure 1:
Representative Feynman diagram for pp→ℓ+νℓγ production with a TGC vertex. |
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Figure 2:
Distributions of the invariant mass of the lepton-photon system in the muon channel (left) and electron channel (right). The electron-induced photon estimate is scaled by a factor of 1.8 in the plot of mℓγ. The uncertainty in the expected yield is the sum of the systematic uncertainties added in quadrature. Wγ refers to the MadGraph-5_aMC@NLO simulation of Wγ. |
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Figure 2-a:
Distribution of the invariant mass of the lepton-photon system in the muon channel. The electron-induced photon estimate is scaled by a factor of 1.8 in the plot of mℓγ. The uncertainty in the expected yield is the sum of the systematic uncertainties added in quadrature. Wγ refers to the MadGraph-5_aMC@NLO simulation of Wγ. |
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Figure 2-b:
Distribution of the invariant mass of the lepton-photon system in the electron channel. The electron-induced photon estimate is scaled by a factor of 1.8 in the plot of mℓγ. The uncertainty in the expected yield is the sum of the systematic uncertainties added in quadrature. Wγ refers to the MadGraph-5_aMC@NLO simulation of Wγ. |
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Figure 3:
The photon pT distribution used for the extraction of limits on dimension-six EFT operators. The last bin includes overflow. |
Tables | |
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Table 1:
Expected and observed number of events. The electron-induced photon estimate is scaled by a factor of 1.8. The uncertainty is the sum of the systematic uncertainties added in quadrature. Wγ refers to the MadGraph-5_aMC@NLO simulation of Wγ. |
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Table 2:
Observed and expected 95% confidence level limits on five dimension-six operator coefficients. The units of the limits are TeV−2. |
Summary |
In conclusion, the inclusive cross section for pp→Wγ production has been measured for the first time at a center-of-mass energy of 13 TeV and with a precision of 4.7%. The measured cross section is σ= 15.58 ± 0.75 pb = 15.58 ± 0.05 (stat) ± 0.73 (exp) ± 0.15 (theory) pb, which is consistent with the MadGraph-5_aMC@NLO in QCD prediction of σ= 15.4 ± 1.2 (scale) ± 0.1 (PDF) pb and below the POWHEG NLO in QCD with NLO competition prediction of σ= 22.4 ± 3.2 (scale) ± 0.1 (PDF) pb. The cross sections separately measured in the electron channel and the muon channel are consistent with each other. The high photon pT part of the photon pT distribution was used to set 95% confidence level limits on dimension-six EFT parameters, including the most stringent limit to date on the coefficient of the lowest dimension CP-even operator that directly alters the WWγ TGC. |
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Compact Muon Solenoid LHC, CERN |
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