![]() | Table of contents: |
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Expected and observed 95% CL upper limits on the product of the VH production cross section times the H → bb branching ratio, with respect to the expectations for a standard model Higgs boson. The median expected limit and the 1- and 2-σ bands are obtained with the LHC CLs method as implemented in RooStats, as are the observed limits at each mass point. The limits are combined for the 2011 7 TeV and the 2012 8 TeV data.
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p-values for background fluctuations to account for the observed excess of events in the data. |
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The most likely value for the production cross section for a 125 GeV standard Higgs boson, relative to the standard model cross section, for each mode and for all modes combined. |
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Dijet invariant mass distribution, combined for all channels, for the high pT(V) bin, for events that pass an event selection optimized for this variable. |
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Same distribution with all backgrounds, except dibosons, subtracted. The solid histograms for the back- grounds and the signal are summed cumulatively. The line histogram for signal and for VV backgrounds are also shown superimposed. The data is represented by points with error bars. |
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VH cartoon |
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BDT output distributions for Z(μμ)H in the low pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(μμ)H in the high pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(ee)H in the low pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(ee)H in the high pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(μν)H in the low pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(μν)H in the high pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(μν)H in the high pT(V) bin with looser b-tagging for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(eν)H in the low pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(eν)H in the high pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for W(eν)H in the high pT(V) bin with looser b-tagging for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(νν)H in the low pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(νν)H in the high pT(V) bin for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distributions for Z(νν)H in the high pT(V) bin with looser b-tagging for data (points with errors), all backgrounds, and signal, after all selection criteria have been applied. |
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BDT output distribution for ZllH in the high pT(V) bin for data (points with errors), all backgrounds and signal, after all selection criteria have been applied. |
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Improvement of the higgs mass resolution in simulated events in cases where at least one of the Higgs jets undergoes a semileptonic b-decay. |
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Validation of the regression performance on data using the Z and jet balance in a Z+bb enriched selection on 8 TeV data. |
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Validation of the regression performance on 8 TeV data using the reconstructed top quark mass in a sample of events selected to enhance single top production. Shapes are shown before and after correction from the application of the regression. The top quark candidate is reconstructed using the b-jet of highest CSV discriminant. |
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Transverse missing energy distribution for ZllH in the low T(V) bin in the dijet mass sideband, control region where the scale factors for the backgrounds are estimated. |
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Transverse momentum of the dijet system in a control region enriched in Z + light flavor quark jets, where the Z decays in to electrons. |
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Projection in the tranverse plane of the Z momentum in a control region enriched in Z + light flavor quark jets, where the Z decays in to muons. |
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Value of the maximum b-tagger between the jets form which the Higgs candidate is formed, in a control region enriched in Z + light flavor quark jets, where the Z decays in to neutrinos. |
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Value of the minimum b-tagger between the jets from which the Higgs candidate is formed, in a control region enriched in Z + light flavor quark jets, where the Z decays in to neutrinos. |