  Run 1 of the LHC has provided three new motivations for supersymmetry: the
need to stabilize the electroweak vacuum, the mass of the Higgs boson, and the
fact that its couplings are Standard Model-like (so far). The prospects for
discovering (and measuring) supersymmetry during future runs of the LHC are
discussed in the frameworks of the constrained MSSM (CMSSM), models with
non-universal soft supersymmetry-breaking contributions to Higgs masses
(NUHM1,2) and the phenomenological MSSM with 10 arbitrary soft
supersymmetry-breaking parameters (pMSSM10). In addition to the classic
searches for missing transverse energy, searches for long-lived charged
sparticles may also be promising. If supersymmetry does show up at the LHC,
there are good prospects for measurements of the spectrum that can be compared
with the indirect indications from other experiments. On the other hand, a
higher-energy future circular proton-proton collider may be the best option for
discovering supersymmetry if it does not appear at the LHC.
