This Letter presents a 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 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 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 chi1 and chi2, and mass-degenerate higgsino-like supersymmetric particles chi1, chi2, chi3. In the limit of a nearly-massless lightest supersymmetric particle chi01, wino-like particles with masses up to 870 and 960 GeV are excluded in the cases of chi02 -> Zchi01 and chi02 -> Hchi01, respectively, and higgsino-like particles are excluded between 300 and 650 GeV.
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
Cappati, A.;Meridiani, P.;Amapane, N.;Argiro';Bellan, R.;Bellora, A.;Costa, M.;Covarelli, R.;Kiani, B.;Migliore, E.;Monteil, E.;Obertino, M. M.;Pacher, L.;Shchelina, K.;Siviero, F.;Sola, V.;Solano, A.;Soldi, D.;Tornago, M.;Vagnerini, A.;Rumerio, P.;Ravera, F.;Salvatico, R.;
2023-01-01
Abstract
This Letter presents a 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 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 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 chi1 and chi2, and mass-degenerate higgsino-like supersymmetric particles chi1, chi2, chi3. In the limit of a nearly-massless lightest supersymmetric particle chi01, wino-like particles with masses up to 870 and 960 GeV are excluded in the cases of chi02 -> Zchi01 and chi02 -> Hchi01, respectively, and higgsino-like particles are excluded between 300 and 650 GeV.File | Dimensione | Formato | |
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