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CMS-SMP-21-001 ; CERN-EP-2022-038
Observation of electroweak W$^{+}$W$^{-}$ pair production in association with two jets in proton-proton collisions at $ \sqrt{s} = $ 13 TeV
PLB 841 (2023) 137495
Abstract: An observation is reported of the electroweak production of a W$^{+}$W$^{-}$ pair in association with two jets, with both W bosons decaying leptonically. The data sample corresponds to an integrated luminosity of 138 fb$ ^{-1} $ of proton-proton collisions at $ \sqrt{s}= $ 13 TeV, collected by the CMS detector at the CERN LHC. Events are selected by requiring exactly two opposite-sign leptons (electrons or muons) and two jets with large pseudorapidity separation and high dijet invariant mass. Events are categorized based on the flavor of the final-state leptons. A signal is observed with a significance of 5.6 standard deviations (5.2 expected) with respect to the background-only hypothesis. The measured fiducial cross section is 10.2 $ \pm $ 2.0 fb and this value is consistent with the standard model prediction of 9.1 $ \pm $ 0.6 fb.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Examples of Feynman diagrams for the EW (left, center) and QCD-induced (right) production of W$^{+}$W$^{-}$ bosons in association with two quarks.

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Figure 1-a:
Example of Feynman diagram for the EW production of W$^{+}$W$^{-}$ bosons in association with two quarks.

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Figure 1-b:
Example of Feynman diagram for the EW production of W$^{+}$W$^{-}$ bosons in association with two quarks.

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Figure 1-c:
Example of Feynman diagram for the QCD-induced production of W$^{+}$W$^{-}$ bosons in association with two quarks.

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Figure 2:
Post-fit DNN output distribution in different-flavor SRs for $ Z_{\ell\ell} < $ 1 (left) and $ Z_{\ell\ell} > $ 1 (right) categories. This variable quantifies how likely each event is signal. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 2-a:
Post-fit DNN output distribution in different-flavor SRs for the $ Z_{\ell\ell} < $ 1 category. This variable quantifies how likely each event is signal. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 2-b:
Post-fit DNN output distribution in different-flavor SRs for the $ Z_{\ell\ell} > $ 1 category. This variable quantifies how likely each event is signal. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 3:
Post-fit $ m_{\mathrm{jj}} $ distribution and number of events in same-flavor ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ combined) SRs for $ Z_{\ell\ell} < $ 1 (left) and $ Z_{\ell\ell} > $ 1 (right) categories. The first two bins contain the number of events in the selected region (as reported in the plots themselves). The third bin contains the number of events in the 300 $ < m_{\mathrm{jj}} $ [GeV] $ < $ 500 and $ |\Delta\eta_{\mathrm{jj}}| > $ 3.5 regions and, for display purposes, is included in the $ m_{\mathrm{jj}} $ distribution, shown in the last five bins. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 3-a:
Post-fit $ m_{\mathrm{jj}} $ distribution and number of events in same-flavor ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ combined) SRs for the $ Z_{\ell\ell} < $ 1 and $ Z_{\ell\ell} > $ 1 category. The first two bins contain the number of events in the selected region (as reported in the plot). The third bin contains the number of events in the 300 $ < m_{\mathrm{jj}} $ [GeV] $ < $ 500 and $ |\Delta\eta_{\mathrm{jj}}| > $ 3.5 regions and, for display purposes, is included in the $ m_{\mathrm{jj}} $ distribution, shown in the last five bins. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 3-b:
Post-fit $ m_{\mathrm{jj}} $ distribution and number of events in same-flavor ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ combined) SRs for the $ Z_{\ell\ell} > $ 1 and $ Z_{\ell\ell} > $ 1 category. The first two bins contain the number of events in the selected region (as reported in the plot). The third bin contains the number of events in the 300 $ < m_{\mathrm{jj}} $ [GeV] $ < $ 500 and $ |\Delta\eta_{\mathrm{jj}}| > $ 3.5 regions and, for display purposes, is included in the $ m_{\mathrm{jj}} $ distribution, shown in the last five bins. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 4:
Post-fit number of events in different-flavor (left) and same-flavor (right, with $ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ combined) CRs. In the left plot, the first bin contains the number of events in the $ {\mathrm{t}\overline{\mathrm{t}}} + \mathrm{t}\mathrm{W} $ different-flavor CR, and the second bin those in the DY $ \tau\tau $ CR. In the right plot, the first bin contains the number of events in the $ {\mathrm{t}\overline{\mathrm{t}}} + \mathrm{t}\mathrm{W} $ same-flavor CR, the second bin those in the $ |\Delta\eta_{\mathrm{jj}}| < $ 5 DY CR, and the third bin those in the $ |\Delta\eta_{\mathrm{jj}}| > $ 5 DY CR. The contributions from background and signal processes (red line) are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 4-a:
Post-fit number of events in the different-flavor CR. The first bin contains the number of events in the $ {\mathrm{t}\overline{\mathrm{t}}} + \mathrm{t}\mathrm{W} $ different-flavor CR, and the second bin those in the DY $ \tau\tau $ CR. The contributions from background and signal processes (red line) are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure 4-b:
Post-fit number of events in the same-flavor (with $ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ combined) CR. The first bin contains the number of events in the $ {\mathrm{t}\overline{\mathrm{t}}} + \mathrm{t}\mathrm{W} $ same-flavor CR, the second bin those in the $ |\Delta\eta_{\mathrm{jj}}| < $ 5 DY CR, and the third bin those in the $ |\Delta\eta_{\mathrm{jj}}| > $ 5 DY CR. The contributions from background and signal processes (red line) are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A1:
Post-fit distributions of $ m_{\mathrm{jj}} $ (upper row) and $ |\Delta\eta_{\mathrm{jj}}| $ (lower row) variables in different-flavor SRs for $ Z_{\ell\ell} < $ 1 (left column) and $ Z_{\ell\ell} > $ 1 (right column) categories. These variables are among the nine observables used as inputs for the DNN, as listed in Table 2. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A1-a:
Post-fit distribution of the $ m_{\mathrm{jj}} $ variable in different-flavor SRs for the $ Z_{\ell\ell} < $ 1 category. This variable is among the nine observables used as inputs for the DNN, as listed in Table 2. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A1-b:
Post-fit distribution of the $ m_{\mathrm{jj}} $ variable in different-flavor SRs for the $ Z_{\ell\ell} > $ 1 category. This variable is among the nine observables used as inputs for the DNN, as listed in Table 2. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A1-c:
Post-fit distribution of the $ |\Delta\eta_{\mathrm{jj}}| $ variable in different-flavor SRs for the $ Z_{\ell\ell} < $ 1 category. This variable is among the nine observables used as inputs for the DNN, as listed in Table 2. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A1-d:
Post-fit distribution of the $ |\Delta\eta_{\mathrm{jj}}| $ variable in different-flavor SRs for the $ Z_{\ell\ell} > $ 1 category. This variable is among the nine observables used as inputs for the DNN, as listed in Table 2. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A2:
Post-fit distribution of the DNN output in different-flavor top CR. Data to SM expectation ratio has some residual shape dependence (less than 5% across the full spectrum), which however was found to not affect the analysis. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A3:
Post-fit distributions of $ m_{\mathrm{jj}} $ (left) and $ |\Delta\eta_{\mathrm{jj}}| $ (right) variables in same-flavor top CR ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ final states combined). The ratio between data and SM expectation is in excellent agreement with 1 within post-fit uncertainties in both spectra. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A3-a:
Post-fit distributions of the $ m_{\mathrm{jj}} $ variable in same-flavor top CR ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ final states combined). The ratio between data and SM expectation is in excellent agreement with 1 within post-fit uncertainties. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.

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Figure A3-b:
Post-fit distributions of the $ |\Delta\eta_{\mathrm{jj}}| $ variable in same-flavor top CR ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ final states combined). The ratio between data and SM expectation is in excellent agreement with 1 within post-fit uncertainties. The contributions from background and signal (red line) processes are shown as stacked histograms; systematic uncertainties are plotted as dashed gray bands. Data points are displayed with asymmetric Poisson vertical bars to ensure a correct statistical coverage all over the spectrum.
Tables

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Table 1:
Post-fit process yields and uncertainties in each SR ($ \mathrm{e}\mathrm{e} $ and $ \mu\mu $ final states combined).

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Table 2:
Set of variables used as inputs to the DNN for both $ Z_{\ell\ell} < $ 1 and $ Z_{\ell\ell} > $ 1 models. The order in the table corresponds to the importance of the discriminating variable for the $ Z_{\ell\ell} < $ 1 model, as obtained through the SHAP method [57,58].

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Table 3:
Sources of systematic uncertainty affecting the cross section measurement by more than 1%. The total uncertainty is also reported, as well as the total systematic and statistical contributions.

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Table 4:
Definition of the fiducial volume similar to the reconstructed SR.

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Table A1:
Summary of the event categorization on top of signal candidates preselection. In each region, same-flavor final states share the same kinematic requirements.
Summary
The EW production of a pair of opposite-sign W bosons in association with two jets has been observed in a data set corresponding to an integrated luminosity of 138 fb$ ^{-1} $ collected with the CMS detector at the CERN LHC in proton-proton collisions at $ \sqrt{s} = $ 13 TeV. Tabulated results are provided in the HEPData record for this analysis [65]. Events containing two opposite-sign leptons (electrons or muons), missing transverse momentum, and two jets with large separation in pseudorapidity and high dijet invariant mass were selected. A deep neural network was employed to deal with the irreducible background from the QCD-induced production of W boson pairs, and the dominant background from the production of $ \mathrm{t} \overline{\mathrm{t}} $ quark pairs. The measured signal corresponds to an observed (expected) significance of 5.6\,(5.2) standard deviations with respect to the background-only hypothesis. The EW W$^{+}$W$^{-}$ production cross section has been measured in two fiducial volumes. In the more inclusive one, the cross section is 99 $ \pm $ 20 fb ( 89 $ \pm $ 5 fb expected), whereas in that comparable with the experimental phase space the measured cross section is 10.2 $ \pm $ 2.0 fb ( 9.1 $ \pm $ 0.6 fb expected). These results are compatible with standard model predictions within one standard deviation.
References
1 D. Espriu and B. Yencho Longitudinal WW scattering in light of the \textquotedblleftHiggs boson\textquotedblright discovery PRD 87 (2013) 055017 1212.4158
2 J. Chang, K. Cheung, C.-T. Lu, and T.-C. Yuan Ww scattering in the era of post-higgs-boson discovery PRD 87 (2013) 093005 1303.6335
3 ATLAS Collaboration Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC PLB 716 (2012) 1 1207.7214
4 CMS Collaboration Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC PLB 716 (2012) 30 CMS-HIG-12-028
1207.7235
5 CMS Collaboration Observation of a new boson with mass near 125 GeV in pp collisions at $ \sqrt{s}= $ 7 and 8 TeV JHEP 06 (2013) 081 CMS-HIG-12-036
1303.4571
6 B. W. Lee, C. Quigg, and H. B. Thacker Weak interactions at very high energies: The role of the Higgs-boson mass PRD 16 (1977) 1519
7 ATLAS Collaboration Evidence for Electroweak Production of $ W^{\pm}W^{\pm}jj $ in pp Collisions at $ \sqrt{s}= $ 8 TeV with the ATLAS Detector PRL 113 (2014) 141803 1405.6241
8 CMS Collaboration Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jets PRL 114 (2014) 051801 CMS-SMP-13-015
1410.6315
9 ATLAS Collaboration Observation of electroweak production of a same-sign W boson pair in association with two jets in pp collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector PRL 123 (2019) 161801 1906.03203
10 CMS Collaboration Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $ \sqrt{s} = $ 13 TeV PRL 120 (2018) 081801 CMS-SMP-17-004
1709.05822
11 CMS Collaboration Measurements of production cross sections of WZ and same-sign WW boson pairs in association with two jets in proton-proton collisions at $ \sqrt{s} = $ 13 TeV PLB 809 (2020) 135710 CMS-SMP-19-012
2005.01173
12 CMS Collaboration Measurements of production cross sections of polarized same-sign W boson pairs in association with two jets in proton-proton collisions at $ \sqrt{s} = $ 13 TeV PLB 812 (2021) 136018 CMS-SMP-20-006
2009.09429
13 R. Bellan et al. A sensitivity study of VBS and diboson WW to dimension-6 EFT operators at the LHC JHEP 05 (2022) 039 2108.03199
14 CMS Collaboration The CMS experiment at the CERN LHC JINST 3 (2008) S08004
15 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
16 CMS Collaboration The CMS trigger system JINST 12 (2017) P01020 CMS-TRG-12-001
1609.02366
17 CMS Collaboration Particle-flow reconstruction and global event description with the CMS detector JINST 12 (2017) P10003 CMS-PRF-14-001
1706.04965
18 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
CDS
19 M. Cacciari, G. P. Salam, and G. Soyez The anti-$ k_{\mathrm{T}} $ jet clustering algorithm JHEP 04 (2008) 063 0802.1189
20 M. Cacciari, G. P. Salam, and G. Soyez FastJet user manual EPJC 72 (2012) 1896 1111.6097
21 CMS Collaboration Pileup mitigation at CMS in 13 TeV data JINST 15 (2020) P09018 CMS-JME-18-001
2003.00503
22 CMS Collaboration Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV JINST 12 (2017) P02014 CMS-JME-13-004
1607.03663
23 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
24 D. Bertolini, P. Harris, M. Low, and N. Tran Pileup per particle identification JHEP 10 (2014) 059 1407.6013
25 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
26 CMS Collaboration CMS luminosity measurement for the 2017 data-taking period at $ \sqrt{s} = $ 13 TeV CMS Physics Analysis Summary, 2017
CMS-PAS-LUM-17-004
CMS-PAS-LUM-17-004
27 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
28 CMS Collaboration Measurements of inclusive W and Z cross sections in pp collisions at $ \sqrt {s} = $ 7 TeV JHEP 01 (2011) 080 CMS-EWK-10-002
1012.2466
29 E. Bols et al. Jet flavour classification using DeepJet JINST 15 (2020) P12012 2008.10519
30 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
31 T. Sjöstrand et al. An introduction to PYTHIA 8.2 Comput. Phys. Commun. 191 (2015) 159 1410.3012
32 B. Cabouat and T. Sjöstrand Some dipole shower studies EPJC 78 (2018) 226 1710.00391
33 B. Jager et al. Parton-shower effects in Higgs production via vector-boson fusion EPJC 80 (2020) 756 2003.12435
34 S. Alioli, P. Nason, C. Oleari, and E. Re A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX JHEP 06 (2010) 043 1002.2581
35 E. Re, M. Wiesemann, and G. Zanderighi NNLOPS accurate predictions for W$ ^+ $W$ ^- $ production JHEP 12 (2018) 121 1805.09857
36 K. Hamilton, P. Nason, and G. Zanderighi Finite quark-mass effects in the NNLOPS POWHEG+MiNLO Higgs generator JHEP 05 (2015) 140 1501.04637
37 S. Bolognesi et al. Spin and parity of a single-produced resonance at the lhc PRD 8 (2012) 095031
38 CMS Collaboration Measurements of properties of the higgs boson in the W boson pair decay channel in proton-proton collisions at $ \sqrt{s}= $ 13 TeV CMS Physics Analysis Summary, 2022
CMS-PAS-HIG-20-013
CMS-PAS-HIG-20-013
39 J. M. Campbell and R. K. Ellis An update on vector boson pair production at hadron colliders PRD 60 (1999) 113006 hep-ph/9905386
40 J. M. Campbell, R. K. Ellis, and C. Williams Vector boson pair production at the LHC JHEP 07 (2011) 017 1105.0020
41 J. M. Campbell, R. K. Ellis, and W. T. Giele A multi-threaded version of MCFM EPJC 75 (2015) 246 1503.06182
42 CMS Collaboration Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV PRD 95 (2017) 092001 CMS-TOP-16-008
1610.04191
43 CMS Collaboration Measurements of differential Z boson production cross sections in proton-proton collisions at $ \sqrt{s}= $ 13 TeV JHEP 12 (2019) 061 CMS-SMP-17-010
1909.04133
44 NNPDF Collaboration Parton distributions with QED corrections NPB 877 (2013) 290 1308.0598
45 NNPDF Collaboration Unbiased global determination of parton distributions and their uncertainties at NNLO and at LO NPB 855 (2012) 153 1107.2652
46 NNPDF Collaboration Parton distributions from high-precision collider data EPJC 77 (2017) 663 1706.00428
47 CMS Collaboration Event generator tunes obtained from underlying event and multiparton scattering measurements EPJC 76 (2016) 155 CMS-GEN-14-001
1512.00815
48 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
49 GEANT 4 Collaboration GEANT 4 -- a simulation toolkit NIM A 506 (2003) 250
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 D. L. Rainwater, R. Szalapski, and D. Zeppenfeld Probing color singlet exchange in Z + two jet events at the CERN LHC PRD 54 (1996) 6680 hep-ph/9605444
53 CMS Collaboration Measurements of properties of the Higgs boson decaying to a W boson pair in pp collisions at $ \sqrt{s}= $ 13 TeV PLB 791 (2019) 96 CMS-HIG-16-042
1806.05246
54 D. P. Kingma and J. Ba Adam: A method for stochastic optimization in 3rd International Conference on Learning Representations, San Diego, 2015
ICLR 201 (2015) 5
1412.6980
55 D. R. Cox The regression analysis of binary sequences J R Stat Soc Series B 20 (1958) 215
56 I. Goodfellow, Y. Bengio, and A. Courville Deep learning MIT Press, 2016
link
57 S. M. Lundberg and S.-I. Lee A unified approach to interpreting model predictions in 31st International Conference on Neural Information Processing Systems, NIPS'17, Red Hook NY, USA, 2017
Proceedings of the 3 (2017) 4768
1705.07874
58 L. S. Shapley A value for n-person games Contributions to the Theory of Games, 1953
link
59 CMS Collaboration Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at $ \sqrt{s} = $ 8 TeV JINST 10 (2015) P06005 CMS-EGM-13-001
1502.02701
60 S. Catani, D. de Florian, M. Grazzini, and P. Nason Soft gluon resummation for Higgs boson production at hadron colliders JHEP 07 (2003) 028 hep-ph/0306211
61 M. Cacciari et al. The $ {\mathrm{t}\overline{\mathrm{t}}} $ cross-section at 1.8 TeV and 1.96 TeV: a study of the systematics due to parton densities and scale dependence JHEP 04 (2004) 068 hep-ph/0303085
62 J. Rojo PDF4LHC recommendations for Run II PoS DIS 018, 2016
link
1606.08243
63 G. Cowan, K. Cranmer, E. Gross, and O. Vitells Asymptotic formulae for likelihood-based tests of new physics EPJC 71 (2011) 1554 1007.1727
64 E. Gross and O. Vitells Trial factors for the look elsewhere effect in high energy physics EPJC 70 (2010) 525 1005.1891
65 CMS Collaboration HEPData record for this analysis link
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