  We investigate topological Cooper pairing, including gapless Weyl and fully
gapped class DIII superconductivity, in a three-dimensional doped Luttinger
semimetal. The latter describes effective spin-3/2 carriers near a quadratic
band touching and captures the normal-state properties of the 227 pyrochlore
iridates and half-Heusler alloys. Electron-electron interactions may favor
non-$s$-wave pairing in such systems, including even-parity $d$-wave pairing.
We argue that the lowest energy $d$-wave pairings are always of complex (e.g.,
$d + i d$) type, with nodal Weyl quasiparticles. This implies $\varrho(E) \sim
|E|^2$ scaling of the density of states (DoS) at low energies in the clean
limit, or $\varrho(E) \sim |E|$ over a wide critical region in the presence of
disorder. The latter is consistent with the $T$-dependence of the penetration
depth in the half-Heusler compound YPtBi. We enumerate routes for experimental
verification, including specific heat, thermal conductivity, NMR relaxation
time, and topological Fermi arcs. Nucleation of any $d$-wave pairing also
causes a small lattice distortion and induces an $s$-wave component; this gives
a route to strain-engineer exotic $s+d$ pairings. We also consider odd-parity,
fully gapped $p$-wave superconductivity. For hole doping, a gapless Majorana
fluid with cubic dispersion appears at the surface. We invent a generalized
surface model with $\nu$-fold dispersion to simulate a bulk with winding number
$\nu$. Using exact diagonalization, we show that disorder drives the surface
into a critically delocalized phase, with universal DoS and multifractal
scaling consistent with the conformal field theory (CFT) SO($n$)${}_\nu$, where
$n \rightarrow 0$ counts replicas. This is contrary to the naive expectation of
a surface thermal metal, and implies that the topology tunes the surface
renormalization group to the CFT in the presence of disorder.
