  An earlier paper showed that it is possible to write down new SUSY Actions in
which it is not possible to define a Supersymmetry Charge. SUSY is defined in
these new Actions by the fact that they satisfy Master Equations. The new SUSY
Actions are very easy to write down. One simply takes a Chiral SUSY Action,
coupled to Gauge and other Chiral Multiplets, and even SuperGravity, if
desired. Then one creates a new Action from this by exchanging all or part of
the Scalar Field $S$ for a new Zinn Source $J$, and the corresponding part of
the Zinn Source $\Gamma$ for a new Antighost Field $\eta$. Since the original
Action satisfies a Master Equation, this exchange guarantees that the new
Action will satisfy the new Master Equation. As was shown in the earlier paper,
the new multiplets have fewer bosonic degrees of freedom than fermionic degrees
of freedom. This is possible because they do not have a Supercharge.
  The resulting new SSM has no need for Squarks or Sleptons. It does not need
spontaneous breaking of SUSY, so that the cosmological constant problem does
not arise (at least at tree level). It mimics the usual non-supersymmetric
Standard Model very well, and the absence of large flavour changing neutral
currents is natural. There is no need for a hidden sector, or a messenger
sector, or explicit `soft' breaking of SUSY. Spontaneous Gauge Symmetry
Breaking implies the existence of two new very heavy Higgs Bosons with mass
13.4 TeV, slightly smaller than the energy of the LHC at 14 TeV. There is also
a curious set of Gauginos and Higgsinos which have exactly the same masses as
the Higgs and Gauge Bosons. These do not couple to the Quarks and Leptons,
except through the Higgs and Gauge Bosons.
