Partially phase-separated liquid-crystal/polymer dispersions display highly fibrillar domain morphologies that are dramatically different from the typical structures found in isotropic mixtures. To explain this, we numerically explore the coupling between phase ordering and phase separation kinetics in model two-dimensional fluid mixtures phase separating into a nematic phase, rich in liquid crystal, coexisting with an isotropic phase, rich in polymer. We find that phase ordering can lead to fibrillar networks of the minority polymer-rich phase.Mixtures of liquid crystals with a small amount of polymer (polymer-stabilized liquid crystals [1][2][3], or PSLC's) show promise for electro-optic devices such as light shutters and displays [4][5][6][7], because the polymer tends to form a network that aligns the liquid crystal [8]. Since polymers and liquid crystals tend to be immiscible, the dispersions are prepared by mixing a small amount of miscible monomer with the liquid crystal and photopolymerizing. As the polymers grow, the system phase separates into an ordered phase rich in liquid crystal and an isotropic phase rich in polymer. Long before the system reaches equilibrium, however, the polymerization "freezes" the mixture into a crosslinked network of polymer-rich domains. Thus, the fabrication of PSLC's involves interplay among three kinetic processes: polymerization, phase separation, and phase ordering. Depending on the time scales that control these processes, a rich variety of morphologies have been observed [9][10][11][12]. Because of the number of nonequilibrium processes involved, however, there is little theoretical understanding of the factors that control the domain morphology. In this Letter, we focus on the interplay between phase separation (PS) and phase ordering (PO) kinetics in mixtures of short, rigid polymers (rods) and long, flexible polymers (coils), as a first step towards rational design and control of the network morphology.It is well known that thermodynamic factors such as the anisotropy of the isotropic/nematic interfacial tension can influence domain morphology, leading to anisotropic domain shapes. However, there are also kinetic factors that control domain morphology, such as the anisotropic diffusion coefficient of a rod. To capture these thermodynamic and kinetic effects, we use a CahnHilliard framework that allows composition and orientational density to evolve in a coupled fashion as functions of position and time following a temperature quench [13]. In contrast to earlier studies that treat orientational density as a scalar order parameter [14,15], this framework includes the orientational density's second-order tensorial nature [16]. Although it is instructive to study the case of two coupled scalar order parameters (Model C [17]), a scalar cannot capture the direction of nematic order. Because a vector does not have head/tail symmetry, it is crucial to retain the tensor order parameter to obtain domain anisotropy [18].To assess the effects of phase ordering, we study two sy...