We consider supersymmetry breaking communicated entirely by the superconfor
mal anomaly in supergravity. This scenario is naturally realized if supersy
mmetry is broken in a hidden sector whose couplings to the observable secto
r are suppressed by more than powers of the Planck scale, as occurs if supe
rsymmetry is broken in a parallel universe living in extra dimensions. This
scenario is extremely predictive: soft supersymmetry breaking couplings ar
e completely determined by anomalous dimensions in the effective theory at
the weak scale. Gaugino and scalar masses are naturally of the same order,
and flavor-changing neutral currents are automatically suppressed. The most
glaring problem with this scenario is that slepton masses are negative in
the minimal supersymmetric standard model. We point out that this problem c
an be simply solved by coupling extra Higgs doublets to the leptons. Lepton
flavor-changing neutral currents can be naturally avoided by approximate s
ymmetries. We also describe more speculative solutions involving compositen
ess near the weak scale. We then turn to electroweak symmetry breaking. Add
ing an explicit mu term gives a value for B mu that is too large by a facto
r of similar to 100. We construct a realistic model in which the mu term ar
ises from the vacuum expectation value of a singlet field, so all weak-scal
e masses are directly related to m(3/2). We show that fully realistic elect
roweak symmetry breaking can occur in this model with moderate fine-tuning.