  Several supersymmetry breaking mechanisms do not produce dimension-3
operators. I show here that this scenario is consistent with present
observations and has several significant virtues: i) When there are no
dimension-3 SUSY-breaking operators there is no SUSY-CP problem. ii)
SUSY-breaking need not occur through gauge singlets, so that the cosmological
problems often encountered in hidden sector SUSY-breaking can be avoided. iii)
Photino and gluino and $R$-hadron masses are naturally consistent with relic
photinos providing the required dark matter density.
  Requiring spontaneous electroweak symmetry implies that scalar masses are
mostly in the $\sim 100$ GeV range. The gluino and photino are massless at tree
level. At 1-loop, the gluino and photino masses at the ew scale are predicted
to be $m_{\gluino}\sim 10 - 600$ MeV and $m_{\photino} \sim 100 - 1400$ MeV.
New hadrons with mass $\sim 1 \frac{1}{2}$ GeV are predicted and described. The
``extra'' flavor singlet pseudoscalar in the $\iota(1440)$ region which has
been observed in several experiments is naturally interpreted as the
mainly-$\gluino \gluino$ bound state which gets its mass via the QCD anomaly.
Its superpartner, a gluon-gluino bound state, would be the lightest $R$-hadron.
For the most interesting portions of parameter space the $R^0$ lifetime is
$10^{-6} - 10^{-10}$ sec, so existing searches would not have been sensitive to
it. Search strategies and other consequences of the scenario are briefly
mentioned.
