RESUMEN
We study a lattice model of a single magnetic polymer chain, where Ising spins are located on the sites of a lattice self-avoiding walk in d=2. We consider the regime where both conformations and magnetic degrees of freedom are dynamic, thus the Ising model is defined on a dynamic lattice and conformations generate an annealed disorder. Using Monte Carlo simulations, we characterize the globule-coil and ferromaget-to-paramagnet transitions, which occur simultaneously at a critical value of the spin-spin coupling. We argue that the transition is continuous-in contrast to d=3 where it is first order. Our results suggest that at the transition the metric exponent takes the θ-polymer value ν=4/7 but the crossover exponent Ï≈0.7, which differs from the expected value for a θ polymer.