7 10 14 E$_{cm}$ (TeV) 10 -2 10 0 10 2 10 4 10 6  (fb) 2 tops 1 top 4 tops 3 tops FIG. 2: Inclusive LO cross sections for multi-top production in the Standard Model with m$_{H}$ = 130 GeV for three LHC center-of-mass energies. Single- and triple-top curves represent the sum over all contributing final states, which are given in Table I. gauge coupling unification, and is characterized by a space-time symmetry that is a natural extension of the Poincar´e group. The generic softly-broken supersymmetric model with the least number of new particles is the Minimal Supersymmetric Standard Model (MSSM). As the MSSM makes no assumptions on the precise method of supersymmetry breaking and instead includes all allowed soft SUSY-breaking terms, many of the parameters defining the masses, mixings, and couplings of the new particles are left undetermined, introducing over 100 arbitrary parameters. The phenomenology of the MSSM is dependent on the choice of these parameters. Spec- ifying the method of SUSY breaking, or choosing parameters with relationships motivated by a particular preference, makes the problem of quantifying MSSM expectations more tractable. The “Snowmass Points and Slopes” (SPS) are a collection of benchmarks derived from different SUSY-breaking methods that all provide viable, and yet markedly different, phenomenological behavior [10]. The parameter point of interest to the current study is SPS 2. This is in the so called “focus point” region of SUSY parameter space [11] and is defined in the mSUGRA model 5