  We revisit the calculation of the electron, neutron, and proton electric
dipole moments (EDMs) in the constrained minimal supersymmetric standard model
(CMSSM). The relatively large mass of the Higgs boson, $m_H \simeq 125$ GeV
coupled with the (as yet) lack of discovery of any supersymmetric particle at
the LHC, has pushed the supersymmetry breaking scale to several TeV or higher.
Though one might expect this decoupling to have relaxed completely any bounds
on the two CP violating phases in the CMSSM ($\theta_\mu$ and $\theta_A$), the
impressive experimental improvements in the limits on the EDMs (particularly
the electron EDM) still allow us to set constraints of order $(0.01 - 0.1)\pi$
on $\theta_A$ and $(0.001 - 0.1)\pi$ on $\theta_\mu$. We also discuss the
impact of future improvements in the experimental limits on supersymmetric
models.
