  In this work, we provide a rigorous definition of ribbon operators in the
Semidual Kitaev lattice model and study their properties. These operators are
essential for understanding quasi-particle excitations within topologically
ordered systems. We show that the ribbon operators generate quasi-particle
excitations at the ends of the ribbon and reveal themselves as irreducible
representations of the Bicrossproduct quantum group
$M(H)=H^{\text{cop}}\lrbicross H$ or $M(H)^{\text{op}}$ depending on their
chirality or local orientation.
