  Folded supersymmetry is a natural theory of the electroweak scale in which
the scalar top partner responsible for canceling the ultraviolet sensitivity of
the Higgs mass at one loop carries no color. As a result, bounds on naturalness
on these theories are more relaxed than in typical supersymmetric models, since
collider bounds on top partners are less stringent. Here we consider the lepton
sector of these theories. We show that a natural realization in a
five-dimensional completion requires the existence of scalar leptons with weak
scale masses and study their phenomenology. We derive bounds on the masses of
these sleptons from the LHC data at $\sqrt{s}=8~$TeV and study the sensitivity
of the $\sqrt{s}=13~$TeV run for various integrated luminosities. When
supersymmetry is broken exclusively by Scherk-Schwarz boundary conditions the
sleptons are stable on collider scales. This leads to bounds on the folded
sleptons that translate into masses above $1~$TeV for the folded stops
resulting in tuning. When additional sources of supersymmetry breaking, which
may be necessary to ensure electroweak symmetry breaking, are allowed the
bounds on stops are mostly avoided. On the other hand, these terms lead to
faster slepton decays resulting in interesting signals with highly displaced
vertices and multi-jet final states inside the detectors.
