“…In this mechanism softening of a ferroelectric TO-phonon mode drives the crystal from a low symmetry C 9 2v (Pna2 1 ) ferroelectric phase to a high symmetry D 16 2h (Pnam) paraelectric phase at ∼288 K [10,30,31,33,35]. We note that several proposals for transitioning to an intermediate phase between 298 and 410 K have also been reported [34,39,40], where the proposed mechanisms [34,41,42] are consistent with models that also show displacive-type phase transition behavior in molecular dynamics simulations [43,44]. Figure 1(a) shows the crystal structure of SbSI in the ferroelectric phase [45] with several unit cells stacked vertically along the crystallographic c axis, which corresponds to the axis of spontaneous polarization [46].…”