When Does a Single Repulsive Dirac Cone Superconduct?

Superconductivity in a single two-dimensional Dirac cone offers a natural route to topological superconductivity. While usually considered extrinsic -- arising from proximity to a conventional superconductor -- we investigate when a doped Dirac cone can spontaneously develop superconductivity from a short-range repulsive interaction $U$ via the Kohn--Luttinger mechanism. We show that an ideal, linear Dirac cone is immune to pairing at leading order in $U^2$. Superconductivity instead emerges only through higher-order in $k$ corrections to the dispersion, which are unavoidable in any lattice realization and crucially dictate the pairing symmetry. The form of the pairing thus reflects how the well-known obstruction to realizing a single Dirac cone on a lattice is circumvented. When a Dirac cone arises from broken time-reversal symmetry -- for instance, at a transition between Chern insulators or in a valley-polarized phase -- we find a topological $p - ip$ state whose chirality is opposite to that of the parent chiral metal above $T_c$. By contrast, for a surface Dirac cone of a 3D topological insulator, superconductivity is stabilized by anisotropies in the dispersion. For $C_{3v}$-symmetric warping, as in $\mathrm{Bi}_{2}\mathrm{Te}_{3}$, pairing is strongest when the Fermi surface becomes hexagonal, leading to order in the $(d \pm id)\times(p+ip)$ channel with accidental near-nodes. In the highly anisotropic limit $v_x \gg v_y$, relevant to side surfaces of layered materials, the Fermi surface splits into two branches, and nesting favors a pairing symmetry $Δ\sim \mathrm{sgn}(k_x)\cos(k_y)$ reminiscent of organic superconductors.