be explained with stop lighter than 2 TeV in this setup. At the same time the stop mass gets an extra Yukawa mediation and maximal stop mixing can be easily realised.

As there is a neutrino Dirac Yukawa contribution to the soft parameters in addition to the ordinary gauge mediation, interesting new physics signature is expected. The mechanism of the charged lepton flavor violation is different from that in mSUGRA [@Borzumati:1986qx] or SUSY GUT [@Ciuchini:2007ha] in which the origin is the running of soft parameters above the See-Saw scale. Though the origin is different, the spectrum looks similar. The crucial difference is that here the flavor violation appearing in lepton doublet soft scalar mass is $16\pi^2$ bigger than the one in mSUGRA. Therefore, the naive expectation is that order one neutrino Dirac Yukawa coupling would be incompatible with the current bounds of various charged lepton flavor violation constraints including $\mu \to e \gamma$.

The computation of the charged lepton flavor violation needs a complete flavor model. Current observation of the charged lepton mass and lepton mixing matrix (PMNS) can be explained in a consistent way with the neutrino Dirac Yukawa matrix which is proportional to the identity matrix. This is 