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The search is motivated by models of supersymmetry that predict the production of neutralinos, the neutral partners of the electroweak gauge and Higgs bosons.  The observed event yields in the signal regions are found to be consistent with the standard model background expectations.  The results are interpreted using simplified models of supersymmetry.  For the electroweak production of nearly degenerate higgsinos, each of whose decay chains yields a neutralino ($\\widetilde{\\chi}^0_1$) that in turn decays to a massless goldstino and a Higgs boson, $\\widetilde{\\chi}^0_1$ masses in the range 175 to 1025 GeV are excluded at 95\\% confidence level.  For the strong production of gluino pairs decaying via a slightly lighter $\\widetilde{\\chi}^0_2$ to H and a light $\\widetilde{\\chi}^0_1$, gluino masses below 2330 GeV are excluded.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t1","@type":"Dataset","description":"Predicted background and observed yields vs bin index","name":"Results"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t2","@type":"Dataset","description":"Cross section 95% CL upper limit vs m($\\widetilde{\\chi}^0_1$) for SMS model TChiHH-G.","name":"Xsec limits, TChiHH-G"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t3","@type":"Dataset","description":"Theory cross sections vs m($\\widetilde{\\chi}^0_1$) for SMS model TChiHH-G.","name":"TChiHH-G_th"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t4","@type":"Dataset","description":"Theory cross sections vs m($\\widetilde{\\chi}^0_1$) for SMS model TChiHH-G, $\\widetilde{\\chi}^0_1, \\widetilde{\\chi}^0_2$ NLSPs only.","name":"TChiHH-G_th_N1N2"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t5","@type":"Dataset","description":"The 95% CL observed and expected upper limits on the production cross sections of the TChiHH signal model as a...","name":"Xsec limits, TChiHH"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t6","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH observed mass limit curve"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t7","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH observed + 1 s.d.(theory) mass limit curve"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t8","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH expected mass limit curve"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t9","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH expected + 1 s.d. mass limit curve"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t10","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH expected + 2 s.d. mass limit curve"},{"@id":"https://doi.org/10.17182/hepdata.114414.v3/t11","@type":"Dataset","description":"Exclusion limits assuming the approximate-NNLO+NNLL cross sections","name":"TChiHH expected - 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