  If supersymmetry (SUSY) is not for stabilizing the electroweak energy scale,
what is it used for in particle physics? We propose that it is for flavor
problems. A cyclic family symmetry is introduced. Under the family symmetry,
only the $\tau$-lepton is massive due to the vacuum expectation value (VEV) of
the Higgs field. This symmetry is broken by a sneutrino VEV which results in
the muon mass. The comparatively large sneutrino VEV does not result in a large
neutrino mass due to requiring heavy gauginos. SUSY breaks at a high scale
$\sim 10^{13}$ GeV. The electroweak energy scale is unnaturally small. No
additional global symmetry, like the R-parity, is imposed. Other aspects of the
model are discussed.
