  Van-Hove (vH) singularities in the vicinity of the Fermi level facilitate the
emergence of electronically mediated Fermi surface instabilities. This is
because they provide a momentum-localized enhancement of density of states
enhancing selective electronic scattering channels. High-temperature
topological superconductivity has been argued for in graphene at vH filling
which, however, has so far proven inaccessible due to the demanded large doping
from pristine half filling. We propose compensated metallicity as a path to
unlock vH-driven pairing close to half filling in an electronic honeycomb
lattice model. It is enabled through the strong breaking of chiral symmetry
from intra-sublattice hybridization, leading to the emergence of a hole pocket
(hp) nearby the van-Hove points $M$ at the Brillouin zone boundary and an
electron pocket (ep) around the zone center $\Gamma$. While the ep is radially
symmetric and barely contributing to the electronic ordering selection, the hp
is dominated by its vH signature and yields electronic order at elevated
scales.
