We provide unambiguous theoretical evidence for the formation of correlation-induced isolated merons in rotationally symmetric quantum dots. Our calculations rely on neither the lowest-Landau-level approximation, nor on the maximum-density-droplet approximation, nor on the existence of a spin-polarized state. For experimentally accessible system parameters, unbound merons condense in the ground state at magnetic fields as low as B * = 0.2 T and for as few as N = 3 confined fermions. The fourfold degenerate ground state at B * corresponds to four orthogonal merons |QC characterized by their topological chirality C and charge Q. This degeneracy is lifted by the Rashba and Dresselhaus spin-orbit interaction, which we include perturbatively, yielding spectroscopic accessibility to individual merons. We further derive a closed-form expression for the topological chirality in the form of a chiral spin current and use it to both characterize our states and predict the existence of other topological textures in other regions of phase space, for example, at N = 5. Finally, we compare the spin textures of our numerically exact meron states to ansatz wave functions of merons in quantum Hall droplets and find that the ansatz qualitatively describes the meron states.