  Two-dimensional transition metal dichalcogenides entwine interaction,
spin-orbit coupling, and topology. Hole-doped systems lack spin degeneracy:
states are indexed with spin and valley specificity. This unique structure
offers new possibilities for correlated phases and phenomena. We realize an
unconventional superconducting pairing phase which is an equal mixture of a
spin singlet and the $m = 0$ spin triplet. It is stable against large in-plane
magnetic fields, and its topology allows quasiparticle excitations of net
nonzero Berry curvature via pair-breaking circularly polarized light.
