  Motivated by Refs \cite{am1,am2}, we analyze how the inflaton decay reheats
the Universe within supersymmetry. In a non-supersymmetric case the inflaton
usually decays via preheating unless its couplings to other fields are very
small. Naively one would expect that supersymmetry enhances bosonic preheating
as it introduces new scalars such as squarks and sleptons. On the contrary, we
point out that preheating is unlikely within supersymmetry. The reason is that
flat directions in the scalar potential, classified by gauge invariant
combinations of slepton and squark fields, are generically displaced towards a
large vacuum expectation value (VEV) in the early Universe. They induce
supersymmetry preserving masses to the inflaton decay products through the
Standard Model Yukawa couplings, which kinematically blocks preheating for VEVs
$> 10^{13}$ GeV. The decay will become allowed only after the flat directions
start oscillating, and once the flat direction VEV is sufficiently redshifted.
For models with weak scale supersymmetry, this generically happens at a Hubble
expansion rate: $H \simeq (10^{-3}-10^{-1}) {\rm TeV}$, at which time the
inflaton decays in the perturbative regime. This is to our knowledge first
analysis where the inflaton decay to the Standard Model particles is treated
properly within supersymmetry. There are number of important consequences: no
overproduction of dangerous supersymmetric relics (particularly gravitinos), no
resonant excitation of superheavy dark matter, and no non-thermal leptogenesis
through non-perturbative creation of the right-handed (s)neutrinos. Finally
supersymmetric flat directions can even spoil hybrid inflation all together by
not allowing the auxiliary field become tachyonic.
