Search for electroweak production of charginos and neutralinos at $\sqrt{s}$ =13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum

The CMS collaboration
Phys.Lett.B 842 (2023) 137460, 2023.

Abstract (data abstract)
Results showing the search for direct production of charginos and neutralinos via electroweak interactions.The results are based on data from proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$ collected with the CMS detector at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$.The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson.These bosons are identified using novel algorithms.No significant excess of events is observed relative to the expectations from the standard model.Limits at the 95\% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$ and $\widetilde{\chi}_{2}^{0}$, and mass-degenerate higgsino-like supersymmetric particles $\widetilde{\chi}_{1}^{\pm}$, $\widetilde{\chi}_{2}^{0}$, and $\widetilde{\chi}_{3}^{0}$.In the limit of a nearly-massless lightest supersymmetric particle $\widetilde{\chi}_{1}^{0}$, wino-like particles with masses up to 870 and $960~\mathrm{GeV}$ are excluded in the cases of $\widetilde{\chi}_{2}^{0}\to\mathrm{Z}\widetilde{\chi}_{1}^{0}$ and $\widetilde{\chi}_{2}^{0}\to\mathrm{H}\widetilde{\chi}_{1}^{0}$, respectively, and higgsino-like particles are excluded between 300 and $650~\mathrm{GeV}$.

  • Figure 3a

    Data from Figure 3 (upper left), located on page 13.

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    SM background prediction vs. observation in the b-veto signal region

  • Figure 3a ratios

    Data from Figure 3 (upper left), located on page 13.

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    SM background observation/prediction in the bVeto signal region

  • Figure 3b

    Data from Figure 3 (upper right), located on page 13.

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    SM background prediction vs. observation in the WH signal region

  • Figure 3b ratios

    Data from Figure 3 (upper right), located on page 13.

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    SM background observation/prediction in the WH signal region

  • Figure 3c

    Data from Figure 3 (lower left), located on page 13.

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    SM background prediction vs. observation in the W signal region

  • Figure 3c ratios

    Data from Figure 3 (lower left), located on page 13.

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    SM background observation/prediction in the W signal region

  • Figure 3d

    Data from Figure 3 (lower right), located on page 13.

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    SM background prediction vs. observation in the H signal region

  • Figure 3d ratios

    Data from Figure 3 (lower right), located on page 13.

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    SM background observation/prediction in the H signal region

  • Figure 4a Observed Lines

    Data from Figure 4 (upper left), located on page 14.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4a Expected Lines

    Data from Figure 4 (upper left), located on page 14.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4a Observed

    Data from Figure 4 (upper left), located on page 14.

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    The 95% CL observed upper limits on the production cross sections for $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^\mp_1$ assuming that each $\widetilde{\chi}^\pm_1$ decays to...

  • Figure 4b Observed Lines

    Data from Figure 4 (upper right), located on page 14.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4b Expected Lines

    Data from Figure 4 (upper right), located on page 14.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4b Observed

    Data from Figure 4 (upper right), located on page 14.

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    The 95% CL observed upper limits on the production cross sections for $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^0_2$ assuming that each $\widetilde{\chi}^\pm_1$ decays to...

  • Figure 4c Observed Lines

    Data from Figure 4 (lower), located on page 14.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4c Expected Lines

    Data from Figure 4 (lower), located on page 14.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 4c Observed

    Data from Figure 4 (lower), located on page 14.

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    The 95% CL observed upper limits on the production cross sections for $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^0_2$ assuming that each $\widetilde{\chi}^\pm_1$ decays to...

  • Figure 5a WW WZ Observed Lines

    Data from Figure 5 (left), located on page 14.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5a WW WZ Expected Lines

    Data from Figure 5 (left), located on page 14.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5a WW WH Observed Lines

    Data from Figure 5 (left), located on page 15.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5a WW WH Expected Lines

    Data from Figure 5 (left), located on page 15.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5b Observed Lines

    Data from Figure 5 (right), located on page 15.

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    Observed exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5b Expected Lines

    Data from Figure 5 (right), located on page 15.

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    Expected exclusion limits assuming the approximate-NLO+NLL cross sections

  • Figure 5b Observed

    Data from Figure 5 (right), located on page 15.

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    The 95% CL observed upper limits on the production cross sections for mass-degenerate higgsino-like$\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^\mp_1$, $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^0_2$, $\widetilde{\chi}^\pm_1$ $\widetilde{\chi}^0_3$ and...

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