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We present the reach of the Large Hadron Collider (LHC) into the parameterspace of No-Scale F-SU(5), starting our analysis with the current operatingenergy of \sqrt{s} = 7 TeV, and extending it on through the bright future of a14 TeV beam. No-Scale F-SU(5) is a model defined by the confluence of theF-lipped SU(5) Grand Unified Theory, two pairs of hypothetical TeV scalevector-like supersymmetric multiplets with origins in F-theory, and thedynamically established boundary conditions of No-Scale Supergravity. Whensearching for a five standard deviation signal, we find that the CMS experimentat the \sqrt{s} = 7 TeV LHC began to penetrate the phenomenologically viableparameter space of this model at just under 1/fb of integrated luminosity, andthat the majority of this space remains intact, subsequent to analyses of thefirst 1.1/fb of CMS data. On the contrary, the ATLAS experiment had not reachedthe F-SU(5) parameter space in its first 1.34/fb of luminosity. Since the CMSand ATLAS detectors have now each amassed a milestone of 5/fb of collectedluminosity, the current LHC is presently effectively probing No-Scale F-SU(5).Upon the crossing of the 5/fb threshold, the 7 TeV LHC will have achieved fivestandard deviation discoverability for a unified gaugino mass of up to about532 GeV, a light stop of 577 GeV, a gluino of 728 GeV, and heavy squarks ofjust over 1 TeV. Extending the analysis to include a future LHC center-of-massbeam energy of \sqrt{s} = 14 TeV, the full model space of No-Scale F-SU(5)should be visible to CMS at about 30/fb of integrated luminosity. We stressthat the F-SU(5) discoverability thresholds discussed here are contingent uponretaining only those events with nine jets or more for the CMS experiment andseven jets or more for the ATLAS experiment.

Prospects for Discovery of Supersymmetric No-Scale F-SU(5) at The Once and Future LHC