  We use conformal field theory to construct model wavefunctions for a gapless
interface between lattice versions of a bosonic Laughlin state and a fermionic
Moore-Read state, both at $\nu=1/2$. The properties of the resulting model
state, such as particle density, correlation function and R\'enyi entanglement
entropy are then studied using the Monte Carlo approach. Moreover, we construct
the wavefunctions also for anyonic excitations (quasiparticles and quasiholes).
We study their density profile, charge and statistics. We show that, similarly
to the Laughlin-Laughlin case studied earlier, some anyons (the Laughlin
Abelian ones) can cross the interface, while others (the non-Abelian ones) lose
their anyonic character in such a process. Also, we argue that, under an
assumption of local particle exchange, multiple interfaces give rise to a
topological degeneracy, which can be interpreted as originating from Majorana
zero modes.
