In critical systems, the e ect of a localized perturbation a ects points that are arbitrarily far away from the perturbation location. In this paper, we study the e ect of localized perturbations on the solution of the random dimer problem in 2𝐷. By means of an accurate numerical analysis, we show that a local perturbation of the optimal covering induces an excitation whose size is extensive with nite probability. We compute the fractal dimension of the excitations and scaling exponents. In particular, excitations in random dimer problems on non-bipartite lattices have the same statistical properties of domain walls in the 2𝐷 spin glass. Excitations produced in bipartite lattices, instead, are compatible with a loop-erased self-avoiding random walk process. In both cases, we nd evidences of conformal invariance of the excitations, that are compatible with SLE 𝜅 with parameter 𝜅 depending on the bipartiteness of the underlying lattice only.