All of the fermions in the Standard Model, with or without right-handed neutrinos, can be modeled with Weyl spinor fields (left-handed or right-handed or a mix of both, it doesn't matter).
There's an isomorphism between Weyl and Majorana spinors in 3+1 dimensions which means that they can also all be modeled with Majorana spinors, according to Howard E. Haber, "Massless Majorana and Weyl fermions cannot be distinguished". (That's an unpublished note, but I believe it's correct.)
A Dirac spinor is two Weyl/Majorana spinors. You can always pair up Weyl/Majorana spinors if you have an even number of them. The naturalness of it depends on how much you can then write operations on the pairs as a unit in the Lagrangian, versus just projecting out the original spinors all the time. In the Standard Model, you can pair up the spinors according to the Higgs "mass" couplings (either leaving the neutrinos unpaired or adding right-handed neutrinos), so that the mass terms look similar to Dirac mass terms, but you then have the $SU(2)\times U(1)$ electroweak symmetry acting asymmetrically on the two halves of the spinors. There's nothing to suggest that the universe is built out of Dirac spinors fundamentally.