The ionic conductivity has been investigated within a wide temperature
and concentration range for the rotator phase fcc-Li2SO4 doped with 0
to 8 mol% MgSO4. For comparison we also measured the ionic conductivi
ty in the melt. For the solid phase the temperature dependence of the
conductivity deviates from the Arrhenius behaviour, but it can be succ
essfully fitted to the Vogel-Tammann-Fulcher (VTF) equation. Also for
the bcc high temperature rotator phases of LiNaSO4 and LiAgSO4 we foun
d that the VTF equation provides a better fit than the Arrhenius equat
ion. The ideal glass transition temperature obtained from the fit to t
he VTF equation is (166+20)degrees C for the fee phase of Li2SO4-MgSO4
, independent of the MgSO4 concentration. For the bcc-phases of LiNaSO
4 and LiAgSO4 it is (113+/-19)degrees C and (135+/-49)degrees C respec
tively. This indicates that although these materials are crystalline,
the ionic conductivity behaves in a similar way to that of an amorphou
s material above the glass transition temperature. For comparison we a
lso reevaluated ionic conductivity data over a wide temperature range
for the archetypical crystalline solid electrolyte, alpha-AgI. As expe
cted, the Arrhenius equation provides an excellent fit in this case si
nce the ionic transport can be described as ionic hopping between avai
lable sites. For the high temperature rotator phases the dynamical dis
order, due to the rotational freedom of the sulphate ions, is thought
to be a key factor for the ionic transport. It is thus suggested that
the free volume model may be used to describe the ionic transport in h
igh temperature rotator phases.