  The Supergravity model named No-Scale ${\cal F}$-$SU(5)$, which is based upon
the flipped $SU$(5) Grand Unified Theory (GUT) with additional TeV-scale
vector-like flippon multiplets, has been partially probed during the LHC Run 1
at 7-8 TeV, though the majority of its model space remains viable and should be
accessible by the 13-14 TeV LHC during Run 2. The model framework possesses the
rather unique capacity to provide a light CP-even Higgs boson mass in the
favored 124-126 GeV window while simultaneously retaining a testably light
supersymmetry (SUSY) spectrum. We summarize the outlook for No-Scale ${\cal
F}$-$SU(5)$ at the 13-14 TeV LHC and review a promising methodology for the
discrimination of its long-chain cascade decay signature. We further show that
proportional dependence of all model scales upon the unified gaugino mass
$M_{1/2}$ minimizes electroweak fine-tuning, allowing the $Z$-boson mass $M_Z$
to be expressed as an explicit function of $M_{1/2}$, $M_Z^2 = M_Z^2
(M_{1/2}^2)$, with implicit dependence upon a dimensionless ratio $c$ of the
supersymmetric Higgs mixing parameter $\mu$ and $M_{1/2}$. Finally, we
elucidate an empirical connection between recent scalar tensor measurements and
No-Scale Supergravity cosmological models that mimic the Starobinsky model of
inflation.
