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Abstract
We investigate the validity of an idea that the Bμ problem is solvable via the renormalization effect in the strongly interacting hidden sector within the gauge mediated supersymmetry breaking scenario. Our analysis starts with a naive boundary condition, which is that the squared scalar masses experience 16π2 suppression. We use softsusy to get the low energy spectra of superparticles with the boundary condition at the scale (ΛCFT) where the hidden sector is integrated out. We visit the low energy spectra and return to ΛCFT where the boundary conditions are given. We find that there is a sign problem, which seems to be generic.
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