  Twisted bilayers of nodal superconductors were recently proposed as a
promising platform to host superconducting phases that spontaneously break
time-reversal symmetry. Here we extend this analysis to twisted multilayers,
focusing on two high-symmetry stackings with alternating ($\pm \theta$) and
constant ($\theta$) twist angles. In analogy to alternating-twist multilayer
graphene, the former can be mapped to twisted bilayers with renormalized
interlayer couplings, along with a remnant gapless monolayer when the number of
layers $L$ is odd. In contrast, the latter exhibits physics beyond twisted
bilayers, including the occurrence of `magic angles' characterized by cubic
band crossings when $L \mod 4 = 3$. Owing to their power-law divergent density
of states, such multilayers are highly susceptible to secondary instabilities.
Within a BCS mean-field theory, defined in the continuum and on a lattice, we
find that both stackings host chiral topological superconductivity in extended
regions of their phase diagrams.
