  The ongoing efforts aiming at control and manipulation of novel topological
phases renewed the interest in bound states induced in superconducting
substrates by magnetic impurities. First described by Yu, Shiba and Rusinov,
those bound states are spin-polarized and exhibit a rather large spatial extent
in two dimensional (2D) materials. Here, using the Bogoliubov--de~Gennes
formalism, we study the Yu--Shiba--Rusinov bound states induced by a
ferromagnetic dimer in 2D triangular lattice. We describe various topographies
of the in-gap bound states, depending on the coupling between impurities and
superconducting host.
