Eutectic dendrites forming in a model ternary system have been studied using the phase-field theory. The eutectic and one-phase dendrites have similar forms, and the tip radius scales with the interface free energy as for one-phase dendrites. The steady-state eutectic patterns appearing on these two-phase dendrites include concentric rings, and single-to multiarm spirals, of which the fluctuations choose, a stochastic phenomenon characterized by a peaked probability distribution. The number of spiral arms correlates with tip radius and the kinetic anisotropy. [7]. In turn, the newly discovered spiraling ternary eutectic dendrites emerge from the interplay of two-phase solidification with the Mullins-Sekerka-type diffusional instability caused by the third component [5]. This spiraling/helical structure has been identified as of interest for creating chiral metamaterials for optical applications via eutectic self-organization [8]. The complex microstructure of some ternary alloys is suspected to originate from eutectic dendrites [9]. Remarkably, multiarm spiraling has been reported experimentally in excitable media [1], in binary eutectics [4], and in Liesegang reactions [10], and theoretically in the FitzHugh-Nagumo model, in which the multiarm spirals form due to the attraction of single spirals [11]. It is yet unclear how general this behavior is, in particular whether multiarm spiraling is possible for ternary eutectic dendrites, and what governs the number of spiraling eutectic arms.In this paper, we show that a minimal phase-field model of ternary freezing is able to describe the spiraling ternary eutectic dendrites, and perform a detailed numerical study of this exotic growth mode. We demonstrate that the multiarm eutectic spiral patterns are robust, so they should be experimentally accessible, and that analogously to the findings for Liesegang reactions [10], the number of spirals results from an interplay of stochastic effects and the competition of nonlinear modes.The free energy of a minimal ternary generalization of the binary phase-field model (see e.g. Ref.[12]) reads as