“…Inclusion of the latent heat contribution from phase-ordering causes the interfacial temperature to approach the bulk transition temperature T b , which subsequently causes the free energy driving force of the isotropic/smectic-A transition to approach zero. Thus, under these conditions, thermal diffusion limits growth resulting in dynamics converging to a power law exponent of n = 1 2 as observed experimentally [33,34,64,65] and predicted theoretically [32,35,66] for liquid crystal growth under shallow quench/undercooling conditions. In the case of metastable nematic pre-ordering, the evolution of the isotropic/metastable nematic front temperature reveals the influence of the latent heat contribution of the trailing smectic-A front.…”