  The proximity-induced spin-triplet $f$-wave symmetry pairing in a monolayer
molybdenum disulfide-superconductor hybrid features an interesting
electron-hole excitations and also effective superconducting subgap, giving
rise to a distinct Andreev resonance state. Owing to the complicated Fermi
surface and momentum dependency of $f$-wave pair potential, monolayer $MoS_2$
with strong spin-orbit coupling can be considered an intriguing structure to
reveal the superconducting state. Actually, this can be possible by calculating
the peculiar spin-valley polarized transport of quasiparticles in a related
normal metal/superconductor junction. We theoretically study the formation of
effective gap at the interface and resulting normalized conductance on top of a
$MoS_2$ under induction of $f$-wave order parameter, using
Bloder-Tinkham-Klapwijk formalism. The superconducting excitations shows that
the gap is renormalized by a \textit{bias limitation} coefficient including
dynamical band parameters of monolayer $MoS_2$, especially, ones related to the
Schrodinger-type momentum of Hamiltonian. The effective gap is more sensitive
to the n-doping regime of superconductor region. The signature of spin-orbit
coupling, topological and asymmetry mass-related terms in the resulting subgap
conductance and, in particular, maximum conductance is presented. In the
absence of topological term, the effective gap reaches to its maximum value.
The unconventional nature of superconducting order leads to the appearance of
zero-bias conductance. In addition, the maximum value of conductance can be
controlled by tuning the doping level of normal and superconductor regions.
