“…We will see in this work that in this regime, the root spin cluster corresponds to a non generic critical Boltzmann map. Kortchemski and Richier [49] proved that, in the bipartite case, the boundary of such random maps converges to the circle C 1 in the scaling limit, agreeing with our result. This result at criticality can shed some light on the link between random maps coupled with an Ising model at the critical temperature and the O √ 2 model in the dilute regime, where interfaces are supposed to be simple in the scaling limit, see for example the papers by Borot, Bouttier, Duplantier and Guitter [12,13,14,15].…”