References

---

[1] Paolo Nason. “A New Method for Combining NLO QCD with Shower Monte Carlo Algorithms.” In: Journal of High Energy Physics 2004.11 (2004), pp. 040–040. doi: 10.1088/1126-6708/2004/11/040. url: https://doi.org/10.1088/1126-6708/2004/11/040.

[2] Stefano Frixione et al. “Matching NLO QCD computations with parton shower simulations: the POWHEG method.” In: Journal of High Energy Physics 2007.11 (2007), pp. 070–070. doi: 10.1088/1126-6708/2007/11/070. url: https://doi.org/10.1088/1126-6708/2007/11/070.

[3] Simone Alioli et al. “A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX.” In: Journal of High Energy Physics 2010.6 (June 2010). doi: 10.1007/jhep06(2010)043. url: https://doi.org/10.1007/jhep06(2010)043 .

[4] Torbjörn Sjöstrand et al. “A brief introduction to PYTHIA 8.1.” In: Computer Physics Communications 178.11 (2008), pp. 852–867.

[5] J De Favereau et al. “DELPHES 3: a modular framework for fast simulation of a generic collider experiment.” In: Journal of High Energy Physics 2014.2 (2014), p. 57.

[6] Pierre Artoisenet, et al., “Unravelling $t\bar{t}H$ via the Matrix Element Method.” In: Physical Review Letters 111.9 (Aug. 2013). doi: 10.1103/physrevlett.111.091802. url: https://doi.org/10.1103/physrevlett.111.091802.

[7] Measurement of $t\bar{t}H$ production in the $H \rightarrow b\bar{b}$ decay channel in 41.5 fb$^{−1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV. Tech. rep. CMS-PAS-HIG-18-030. Geneva:CERN, 2019. url: https://cds.cern.ch/record/2675023 .

[8] Measurement of the Higgs boson decaying to b-quarks produced in association with a top-quark pair in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector. Tech. rep. ATLAS-CONF-2020-058. Geneva: CERN, 2020. url: https://cds.cern.ch/record/2743685.

[9] Matteo Cacciari et al. “The anti-ktjet clustering algorithm.” In: Journal of High Energy Physics 2008.04 (2008), pp. 063–063. doi:10.1088/1126-6708/2008/04/063.url: https://doi.org/10.1088/1126-6708/2008/04/063.