CMS-PAS-B2G-20-001 | ||
Search for resonances decaying to triple W-boson final states in proton-proton collisions at $\sqrt{s}= $ 13 TeV | ||
CMS Collaboration | ||
April 2021 | ||
Abstract: The first search for resonances decaying into a radion and a W boson in proton-proton collision data recorded by the CMS detector at $\sqrt{s} = $ 13 TeV corresponding to an integrated luminosity of 137 fb$^{-1}$ is reported. The radion is reconstructed through its decay into two W bosons. We require the presence of one isolated lepton and missing transverse momentum from a leptonic W boson decay, and either one or two massive large-radius jets containing the decay products of the other two W bosons. No excess over the background estimation is observed and upper limits are set on model parameters. | ||
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These preliminary results are superseded in this paper, Submitted to PRL. The superseded preliminary plots can be found here. |
Figures | |
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Figure 1:
Feynman-like diagrams for the decay of a Kaluza-Klein excitation resonance $ {{\rm W}_{\mathrm {KK}}}$ decaying to the final states considered in this analysis. Left: three individually reconstructed W bosons; right: one individually reconstructed W boson and two W bosons reconstructed as a single large-radius jet. |
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Figure 2:
Leading jet mass $ {{\rm M}_{{\rm j}}}$ for a triboson signal with $ {{\rm M}_{{{\rm W}_{\mathrm {KK}}}}} = $ 3.5 TeV and $ {{\rm M}_{{\mathrm {R}}}} = $ 0.21 TeV split into the different signal categories and normalized to the theoretical prediction for the signal production cross section. The percentages indicated in the legend correspond to the relative category fractions for this signal point. |
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Figure 3:
The deep-WH discriminant for a triboson signal with $ {{\rm M}_{{{\rm W}_{\mathrm {KK}}}}} = $ 3.5 TeV and $ {{\rm M}_{{\mathrm {R}}}} = $ 0.21 TeV split into the different signal categories (dashed and dotted lines) and for jets from background processes (full line). |
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Figure 4:
Background-only post-fit distribution of the reconstructed $\ell \nu $+jets system ${{\rm M}_{\mathrm {jj\ell}\nu}}$ in data and simulation for SR4. The shape of a triboson signal with $ {{\rm M}_{{{\rm W}_{\mathrm {KK}}}}} = $ 2.5 TeV and $ {{\rm M}_{{\mathrm {R}}}} = $ 1 TeV is shown in violet. |
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Figure 5:
Pull (Data$-$Prediction$/\sigma _{\mathrm {stat}}$) distributions of the background-only fit to the reconstructed $\ell \nu $+jets system ${{\rm M}_{\mathrm {j\ell}\nu}} ({{\rm M}_{\mathrm {jj\ell}\nu}})$ for all SRs. Post-fit systematic uncertainties are indicated by the shaded bands. Exemplary signal points normalized to the theoretical prediction for the signal production cross section are shown using full and dashed lines. |
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Figure 6:
Expected and observed upper limits at 95% CL on the signal cross section as functions of the ${{\rm W}_{\mathrm {KK}}} and {\mathrm {R}}$ resonance masses. |
Summary |
In summary, we have presented for the first time a search for resonances decaying in cascade through ${{\rm W}_{\mathrm {KK}}} \rightarrow \mathrm{W}\mathrm{R}$ and $\mathrm{R} \rightarrow \mathrm{W}\mathrm{W}$ to three W bosons, where ${{\rm W}_{\mathrm {KK}}}$ is a Kaluza-Klein excited massive gauge boson and R is a scalar radion. The search has been performed in proton-proton collision data at a center-of-mass energy of 13 TeV, corresponding to total integrated luminosity of 137 fb$^{-1}$. The final states analyzed manifest themselves in one isolated lepton, missing transverse momentum, and one or two massive large radius jets. Both regimes with two W bosons merged in a single WW jet and with two separated W boson jets are simultaneously probed. Results are found to agree with the predictions of the standard model. Limits are set on model parameters, which are the first on the production of triboson resonances at the LHC. |
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Compact Muon Solenoid LHC, CERN |