Consider (mod 1) acting on , a Lipschitz potential $A:S^1 \to 0<\lambda<1b_\lambda:S^1 \to b_\lambda(x) = \max_{T(y)=x} { \lambda , b_\lambda(y) + A(y)}.\lambda \to 1b_\lambda- \frac{m(A)}{1-\lambda}V(x) = \max_{\mu \in } \int S(y,x) , d \mu(y)S$ is the Ma~ne potential, is the set of invariant probabilities with support on the Aubry set and . For and , there exists a unique fixed point for the equation $e^{u_{\lambda,\beta}(x)} = \sum_{T(y)=x}e^{\beta A(y) +\lambda u_{\lambda,\beta}(y)}$. It is known that as the family $e^{[u_{\lambda,\beta}- \sup u_{\lambda,\beta}]}\phi_\beta \beta A$. We consider , and , as . Under these hypothesis we will show that converges uniformly to the above , as . The parameter represents the inverse of temperature in Statistical Mechanics and means that we are considering that the temperature goes to zero. Under these conditions we get selection of subaction when .

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