  In this paper we consider the additive logarithmic finite strain plasticity
formulation from the view point of loss of ellipticity in elastic unloading. We
prove that even if an elastic energy $F\mapsto W(F)=\hat{W}(\log U)$ defined in
terms of logarithmic strain $\log U$, where $U=\sqrt{F^T\, F}$, is everywhere
rank-one convex as a function of $F$, the new function $F\mapsto
\widetilde{W}(F)=\hat{W}(\log U-\log U_p)$ need not remain rank-one convex at
some given plastic stretch $U_p$ (viz. $E_p^{\log}:=\log U_p$). This is in
complete contrast to multiplicative plasticity in which $F\mapsto W(F\,
F_p^{-1})$ remains rank-one convex at every plastic distortion $F_p$ if
$F\mapsto W(F)$ is rank-one convex. We show this disturbing feature with the
help of a recently considered family of exponentiated Hencky energies.
