fits for individual models versus the CMS data. For the bottom plot the cross sections have been scaled by $p_{T}^{5}$ to better see the differences between the models.\[fig:central\]](Central "fig:"){width="48.00000%"} ![The $p_{T}$ spectra of the central jet calculated using the best fits for individual models versus the CMS data. For the bottom plot the cross sections have been scaled by $p_{T}^{5}$ to better see the differences between the models.\[fig:central\]](Central_scaled "fig:"){width="48.00000%"}

![The $p_{T}$ spectra of the forward jet calculated using the best fits for individual models versus the CMS data. For the bottom plot the cross sections have been scaled by $p_{T}^{5}$ to better see the differences between the models.\[fig:forward\]](Forward "fig:"){width="48.00000%"} ![The $p_{T}$ spectra of the forward jet calculated using the best fits for individual models versus the CMS data. For the bottom plot the cross sections have been scaled by $p_{T}^{5}$ to better see the differences between the models.\[fig:forward\]](Forward_scaled "fig:"){width="48.00000%"}

The influence of the Sudakov resummation model is illustrated in Fig. \[fig:sudeffect\]. Here, we have chosen the best fits to illustrate the effect. We see, that the jet spectra are rather weakly affected by the resummation, although the forward jet spectrum becomes steeper than the data.

![An effect of the Sudakov 