  Recoverable strain is the strain recovered once a stress is removed from a
body, in the direction opposite to that in which the stress had acted. To date,
the phenomenon has been understood as being elastic in origin: polymer chains
stretched in the direction of an imposed stress will recoil after the stress is
removed, for example. Any unrecoverable strain is instead attributed to
irreversible plastic deformations. Here we study theoretically recoverable and
unrecoverable strain within the soft glassy rheology model, aimed at describing
the rheology of elastoplastic yield stress fluids and amorphous soft solids. We
consider a material subject to the switch-on of a shear stress that is held
constant before later being set back to zero, after which the strain recovery
is observed. After an initially fast recoil that is indeed elastic in nature,
consistent with the usual intuition, we find that significant subsequent strain
recovery then arises not via further recoil of elasticity but instead by
`reverse plasticity', in a sense that we discuss carefully. Also unexpectedly,
although in rare parameter regimes, this plastic part of the strain post
switch-off does not always in fact recover in the negative direction, counter
to that of the previously imposed stress, but can sometimes continue to
accumulate in the forward direction. The recovery is then non-monotonic
overall, reminiscent of recent observations of non-monotonic stress relaxation
after straining, which have been attributed to complex material memory effects.
We elucidate the mechanisms underlying these behaviours in terms of the
evolution of the SGR model's population of elastoplastic elements, and suggest
connections with the notion of `reversible plasticity', as discussed in the
recent physics literature.
