the `HLT_PFJet320` trigger (Table \[tab:DataSamples\]). The study of a larger data-set was beyond the available computing resources. The integrated luminosity has been calculated using the public available GoodRun-List as well as the corresponding tools. In total, 831,662 triggered events, which pass the GoodRun-List requirement, are used in this analysis.

[l | l | c]{} Data stream / Trigger name & Dataset Name & $\int L dt $ $[\ipb]$\
Incl. Jet-Triggers / `Trigger_HLT_PFJet320` & JetHT\_Run2012C [@CMS:QCDData] & 289 / 166\

An overview of the various signal and background Monte Carlo (MC) samples used in this analysis is given in Table \[tab:MCSamples\], indicating the underlying physics process, the dataset name and the corresponding inclusive cross-section. The inclusive QCD MC was generated with <span style="font-variant:small-caps;">Pythia6</span> [@Sjostrand:2006za] and covers a jet transverse momentum range between 50 and 3000 GeV. In addition, a 4-jet sample is used as alternative QCD sample, which is based on the <span style="font-variant:small-caps;">Alpgen</span> generator [@Mangano:2002ea]. The Drell-Yan processes (W/Z) in the muon decay channel were generated using with the <span style="font-variant:small-caps;">PowhegBox</span> Monte Carlo program [@Alioli:2008gx; @Alioli:2010xd] interfaced to the <span style="font-variant:small-caps;">Pythia</span> v.6.4.26  [@Sjostrand:2006za] parton shower model. All other processes are modeled with the tree-level matrix element event generator <span style="font-variant:small-caps;">MadGraph</span> 