Table 1.
Summary information on the analyses included in this paper. The column “H production” indicates the production mechanism targeted by an analysis; it does not imply 100 % purity. The main contribution in the untagged and inclusive categories is always gluon fusion. The (jj)VBF refers to dijet pair consistent with the VBF topology, and (jj)W(Z) to a dijet pair with an invariant mass consistent with coming from a W (Z) dijet decay. For the WW→ℓνℓν and ZZ→2ℓ2ℓ′ channels the full possible mass range starts from 110 GeV, but in this paper both analyses are restricted to the masses above 145 GeV. The ZZ→2ℓ2q analysis uses only 7 TeV data. The notation “((ee,μμ),eμ)+(0 or 1 jets)” indicates that the analysis is performed in two independent lepton categories (ee,μμ) and (eμ), each category further subdivided in two subcategories with zero or one jets, thus giving a total of four independent channels
| H decay mode | H production | Exclusive final states | No. of channels | m H range [GeV] | m H resolution |
|---|---|---|---|---|---|
| WW→ℓνℓν | 0/1-jets | ((ee,μμ),eμ)+(0 or 1 jets) | 4 | 145–600 | 20 % |
| WW→ℓνℓν | VBF tag | ((ee,μμ),eμ)+(jj)VBF | 2 | 145–600 | 20 % |
| WW→ℓνqq | Untagged | (eν,μν)+((jj)W with 0 or 1 jets) | 4 | 180–600 | 5–15 % |
| ZZ→2ℓ2ℓ′ | Inclusive | 4e, 4μ, 2e2μ | 3 | 145–1000 | 1–2 % |
| (ee,μμ)+(τ h τ h,τ e τ h,τ μ τ h,τ e τ μ) | 8 | 200–1000 | 10–15 % | ||
| ZZ→2ℓ2q | Inclusive | (ee,μμ)+((jj)Z with 0, 1, 2b-tags) | 6 | 200–600 | 3 % |
| ZZ→2ℓ2ν | Untagged | (ee,μμ)+0, 1, 2 non-VBF jets | 6 | 200–1000 | 7 % |
| ZZ→2ℓ2ν | VBF tag | (ee,μμ)+(jj)VBF | 2 | 200–1000 | 7 % |