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implemented with the “usermod” format and the cross section for the three-top final state is found directly. For the MSSM we use the standard MadGraph MSSM implementation and the parameter card for SPS 2 from the MadGraph webpage $^{2}$. We calculate the cross section for the on-shell gluino pair and then determine the triple-top cross section using the branching fractions in Table II. The results for three different LHC running energies are given in Table III and the sum of all processes for each model is plotted with the SM results in Figure 5(a). 

At each energy studied, the new physics models lie approximately an order of magnitude 

