CMS-PAS-HIG-24-001 | ||
Search for HHWW couplings in the VBS production of W±W±H, with H→bˉb decays | ||
CMS Collaboration | ||
27 July 2024 | ||
Abstract: A search is performed for anomalous HHWW couplings based on the process pp→W±W±H+jj, using proton-proton collision data collected by the CMS experiment at a center-of-mass energy of √s= 13 TeV in the LHC Run 2, corresponding to a total integrated luminosity of 138 fb−1. The search is performed in final states that contain a forward-backward jet pair, two W bosons that decay to same-sign leptons, and a Higgs boson that decays into two bottom quarks. Boosted decision trees are trained to separate the signal from the background. The HHWW coupling modifier κWW is constrained at 95% confidence level to be in the interval [−3.3,5.3], consistent with the expected interval of [−2.4,4.4]. | ||
Links: CDS record (PDF) ; CADI line (restricted) ; |
Figures | |
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Figure 1:
Tree-level Feynman diagrams of vector boson scattering multi-boson productions with Higgs boson in the final state, with (a) related to the Higgs self-coupling (κλ), and (b) related to the Higgs gauge quartic coupling (κVV). |
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Figure 1-a:
Tree-level Feynman diagrams of vector boson scattering multi-boson productions with Higgs boson in the final state, with (a) related to the Higgs self-coupling (κλ), and (b) related to the Higgs gauge quartic coupling (κVV). |
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Figure 1-b:
Tree-level Feynman diagrams of vector boson scattering multi-boson productions with Higgs boson in the final state, with (a) related to the Higgs self-coupling (κλ), and (b) related to the Higgs gauge quartic coupling (κVV). |
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Figure 2:
Data-MC comparison of mjj and Δηjj distributions in the pre-selection regions. Two signal hypotheses, with one for κVV= 1 which represents the SM and the other for κVV= 4.5, are plotted. The uncertainty band in the ratio plots represents the pre-fit statistical uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 2-a:
Data-MC comparison of mjj and Δηjj distributions in the pre-selection regions. Two signal hypotheses, with one for κVV= 1 which represents the SM and the other for κVV= 4.5, are plotted. The uncertainty band in the ratio plots represents the pre-fit statistical uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 2-b:
Data-MC comparison of mjj and Δηjj distributions in the pre-selection regions. Two signal hypotheses, with one for κVV= 1 which represents the SM and the other for κVV= 4.5, are plotted. The uncertainty band in the ratio plots represents the pre-fit statistical uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 3:
Post-fit shapes for the SR, including (a) ℓℓ final state (b) ℓτ final state. The uncertainty band in the ratio plots represents the post-fit uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 3-a:
Post-fit shapes for the SR, including (a) ℓℓ final state (b) ℓτ final state. The uncertainty band in the ratio plots represents the post-fit uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 3-b:
Post-fit shapes for the SR, including (a) ℓℓ final state (b) ℓτ final state. The uncertainty band in the ratio plots represents the post-fit uncertainty of the Monte Carlo, which corresponds to the uncertainty band in the distribution plots. |
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Figure 4:
Limits of κVV with CL=95%. |
Tables | |
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Table 1:
Input variables used for the event kinematics BDT. |
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Table 2:
The post-fit yields of the CR, for ℓℓ and ℓτ categories separately. The errors for total background include the statistical and systematic uncertainties. |
Summary |
Data recorded with the CMS experiment during LHC Run 2 amounting to 138 fb−1 of pp collisions at √s= 13 TeV are used to search for anomalous couplings in the process pp→W±W±H+jj, where the Higgs boson decays to two bottom quarks and the W bosons decay leptonically. The analysis focuses on the channel in which the two b-jets are merged. The observed(expected) 95% CL interval for κWW is [−3.3,5.3]([−2.4,4.4]). This marks the first analysis of the pp→W±W±H+jj process and opens the possibility of further analysis of the same process with different final states. |
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Compact Muon Solenoid LHC, CERN |
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