Abstract
The production of dijets in association with a Z-boson (Z\(_{\text {jj}}\) production) is dominated by the Drell-Yan process, with the additional jets arising as a result of the strong interaction.
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Notes
- 1.
\(\mathrm{p}_{\mathrm{T}}^\mathrm{balance}\) is defined as:
$$\begin{aligned} \mathrm{p}_{\mathrm{T}}^\mathrm{balance}= \frac{(p^{l_1}+p^{l_2} + p^{j_1} + p^{j_2})_\mathrm{T}}{\mathrm{p}_{\mathrm{T}}^{l_1} + \mathrm{p}_{\mathrm{T}}^{l_2} + \mathrm{p}_{\mathrm{T}}^{j_1} + \mathrm{p}_{\mathrm{T}}^{j_2}} \end{aligned}$$(7.1)where \(l_1\) and \(l_2\) label the two leptons which make up the Z-boson candidate.
- 2.
In the EWUnfolding package the default procedure treats the correction factors like efficiencies, and the binomial uncertainty equation is used, \(\sigma \,\)=\(\,\sqrt{\epsilon (1-\epsilon )/N}\). However, these correction factors are not true efficiencies and in principle could have values larger than 1.
- 3.
Apart from the differential cross section as a function of \(|\Delta {y}|\) in the search and control phase spaces, all distributions are fit across their entire range. The differential cross section as a function of \(|\Delta {y}|\) in these phase spaces has an unusual shape and is difficult to fit. Therefore the fit is performed in the steeply-falling region 3Â \(<\)Â \(|{\Delta }y|\)Â \(<\)Â 8, where statistics are lower and the smoothing procedure becomes more important.
- 4.
\(\sigma _\mathrm{{toy}}\) is either added or taken away from \(\mu _\mathrm{{toy}}\) to produce the largest difference with respect to the nominal \(N_\mathrm{EW}\).
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Joshi, K. (2015). Measurements of Electroweak Z Boson + Dijet Production. In: QCD Radiation in Top-Antitop and Z+Jets Final States. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-19653-4_7
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