  Motivated by theory and experiments on strain induced pseudo-Landau levels
(LLs) of Dirac fermions in graphene and topological materials, we consider its
extension for Bogoliubov quasiparticles (QPs) in a nodal superconductor (SC).
We show, using an effective low energy description and numerical lattice
calculations for a d-wave SC, that a spatial variation of the electronic
hopping amplitude or a spatially varying s-wave pairing component can act as a
pseudo-magnetic field for the Bogoliubov QPs, leading to the formation of
pseudo-LLs. We propose realizations of this phenomenon in the cuprate SCs, via
strain engineering in films or nanowires, or s-wave proximity coupling in the
vicinity of a nematic instability, and discuss its signatures in tunneling
experiments.
