Table 5 Breakdown of contributions to the uncertainty in the fitted values of \(\mu _{VH(c{\bar{c}})}\), \(\mu _{VW(cq)}\) and \(\mu _{VZ(c{\bar{c}})}\). The sum in quadrature of uncertainties from different sources may differ from the total due to correlations. In cases where the upward and downward systematic variations have different values, the mean of the absolute values is shown
Source of uncertainty | \(\mu _{VH(c{\bar{c}})}\) | \(\mu _{VW(cq)}\) | \(\mu _{VZ(c{\bar{c}})}\) | |
|---|---|---|---|---|
Total | 15.3 | 0.24 | 0.48 | |
Statistical | 10.0 | 0.11 | 0.32 | |
Systematic | 11.5 | 0.21 | 0.36 | |
Statistical uncertainties | ||||
Signal normalisation | 7.8 | 0.05 | 0.23 | |
Other normalisations | 5.1 | 0.09 | 0.22 | |
Theoretical and modelling uncertainties | ||||
\(VH(\rightarrow c{\bar{c}})\) | 2.1 | \( <0.01 \) | 0.01 | |
\(\text {Z}\,+\,\text {jets}\) | 7.0 | 0.05 | 0.17 | |
Top quark | 3.9 | 0.13 | 0.09 | |
\(\text {W}\,+\,\text {jets}\) | 3.0 | 0.05 | 0.11 | |
Diboson | 1.0 | 0.09 | 0.12 | |
\(VH(\rightarrow b{\bar{b}})\) | 0.8 | \( <0.01 \) | 0.01 | |
Multi-jet | 1.0 | 0.03 | 0.02 | |
Simulation samples size | 4.2 | 0.09 | 0.13 | |
Experimental uncertainties | ||||
Jets | 2.8 | 0.06 | 0.13 | |
Leptons | 0.5 | 0.01 | 0.01 | |
\(E_{\text {T}}^{\text {miss}}\) | 0.2 | 0.01 | 0.01 | |
Pile-up and luminosity | 0.3 | 0.01 | 0.01 | |
Flavour tagging | c-jets | 1.6 | 0.05 | 0.16 |
b-jets | 1.1 | 0.01 | 0.03 | |
light-jets | 0.4 | 0.01 | 0.06 | |
\(\tau \)-jets | 0.3 | 0.01 | 0.04 | |
Truth-flavour tagging | \(\Delta R\) correction | 3.3 | 0.03 | 0.10 |
Residual non-closure | 1.7 | 0.03 | 0.10 | |