We recompute the one-loop effective potential in supergravity and use this to compute the gravitational backreaction on the global vacuum [^1]. The perturbations are shown to be small, as one expects from gravitational corrections, but non-trivial. We stress that it is necessary to consider gravitational corrections, even though we know they are small. They are important when determining the expectation values of the fields, most notably the moduli, but the remaining fields are shifted more than dimesional analysis would suggest. The most interesting effect is the generation of non-zero, but Planck suppressed, F-terms for the magnetic quarks. Hence, there appear two distinct scales in the sector that breaks supersymmetry.

It is interesting to calculate the relative importance of several mediation mechanisms in this setup, specifically anomaly, gravity and gauge mediation. We give order of magnitude estimates for the soft masses spectrum generated by these three mechanisms and argue that the spectrum can have a striking gap between the gaugino masses and the soft scalar masses. This is reminiscent of split SUSY [@ArkaniHamed:2004fb], but the split is not allowed to be arbitrarily large since it is constrained by the requirement that $V=0$ in the meta-stable minimum.

We note that setting $V=0$ 