Naturalness of electroweak symmetry breaking in weak scale supersymmetric
theories may suggest the absence of the conventional supersymmetric desert. We
present a simple, realistic framework for supersymmetry in which (most of) the
virtues of the supersymmetric desert are naturally reproduced without having a
large energy interval above the weak scale. The successful supersymmetric
prediction for the low-energy gauge couplings is reproduced due to a gauged R
symmetry present in the effective theory at the weak scale. The observable
sector superpotential naturally takes the form of the next-to-minimal
supersymmetric standard model, but without being subject to the Landau pole
constraints up to the conventional unification scale. Supersymmetry breaking
masses are generated by the F-term and D-term VEVs of singlet and U(1)_R gauge
fields, as well as by anomaly mediation, at a scale not far above the weak
scale. We study the resulting patten of supersymmetry breaking masses in
detail, and find that it can be quite distinct. We construct classes of
explicit models within this framework, based on higher dimensional unified
theories with TeV-sized extra dimensions. A similar model based on a non-R
symmetry is also presented. These models have a rich phenomenology at the TeV
scale, and allow for detailed analyses of, e.g., electroweak symmetry breaking.Comment: 42 page