Visible effects of the hidden sector

The renormalization of operators responsible for soft supersymmetry breaking is usually calculated by starting at some high scale and including only visible sector interactions in the evolution equations, while ignoring hidden sector interactions. Here we explain why this is correct only for the most trivial structures in the hidden sector and discuss possible implications. This investigation was prompted by the idea of conformal sequestering. In that framework hidden sector renormalizations by nearly conformal dynamics are critical. In the original models of conformal sequestering it was necessary to impose hidden sector flavor symmetries to achieve the sequestered form. We present models that can evade this requirement and lead to no-scale or anomaly mediated boundary conditions, but the necessary structures do not seem generic. More generally, the ratios of scalar masses to gaugino masses, the $\mu$ term, the $B\mu$ term, A terms, and the gravitino mass can be significantly affected.