  We show the presence of non-relativistic L\'evy-Leblond fermions in flat
three- and four-layers graphene with AB stacking, extending the results
obtained in [Curvatronics2017] for bilayer graphene. When the layer is curved
we obtain a set of equations for Galilean fermions that are a variation of
those of L\'evy-Leblond with a well defined combination of pseudospin, and that
admit L\'evy-Leblond spinors as solutions in an approriate limit. The local
energy of such Galilean fermions is sensitive to the intrinsic curvature of the
surface. We discuss the relationship between two-dimensional pseudospin,
labelling layer degrees of freedom, and the different energy bands. For
L\'evy-Leblond fermions an interpretation is given in terms of massless
fermions in an effective 4D spacetime, and in this case the pseudospin is
related to four dimensional chirality. A non-zero energy band gap between
conduction and valence electronic bands is obtained for surfaces with positive
curvature.
