  When the interface of a superconductor (SC) with Weyl semimetal (WSM)
supports Fermi arcs, the chirality blockade eliminates the induction of
superconductivity into the bulk. This leaves the Fermi arc states as the only
low-energy degrees of freedom in the proximity problem. Therefore the SC|WSM
system will be a platform to probe transport properties that only involve the
Fermi arcs. With a boundary condition that flips the spin at the boundary, we
find a $Z_2$ protected Bogoliubov Fermi contour (BFC) around which the
Bogoliubov quasi-particles disperse linearly. The resulting BFC and excitations
around it leave a distinct $T^2$ temperature dependence in their contribution
to specific heat. Furthermore, the topologically protected BFC being a Majorana
Fermi surface gives rise to a zero-bias peak the strength of which
characteristically depends on the length of Fermi arc and tunneling strength.
For the other BC that flips the chirality at the interface, instead of BFCs we
have Bogoliubov- Weyl nodes whose location depends on the tunneling strength.
