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SELECTION OF CALIBRATED SUBACTION WHEN TEMPERATURE GOES TO ZERO IN THE DISCOUNTED PROBLEM

机译:在打折问题中,当温度趋于零时,选择校准的反应

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Consider T(x) = dx (mod 1) acting on S-1, a Lipschitz potential A : S-1 -> R, 0 < lambda < 1 and the unique function b(lambda ): S-1 -> R satisfying b(lambda)(x) = max(T(y)=x){lambda b(lambda)(y) + A(y)}.We will show that, when lambda -> 1, the function b(lambda) - m(A)/1-lambda converges uniformly to the calibrated subaction V(x) = max(mu is an element of M) integral S(y,x) d mu(y), where S is the Mane potential, M is the set of invariant probabilities with support on the Aubry set and m(A) = sup(mu is an element of M) integral Ad mu.For beta > 0 and lambda is an element of (0,1), there exists a unique fixed point u(lambda,beta) : S-1 -> R for the equation e(u lambda,beta(x)) = Sigma(T(y)())(=x)e(beta A(y)+lambda u lambda,beta(y)). It is known that as lambda -> 1 the family e([u lambda,beta-supu lambda,beta]) converges uniformly to the main eigenfuntion phi(beta) for the Ruelle operator associated to beta A. We consider lambda = lambda(beta), beta(1 - lambda(beta)) -> +infinity and lambda(beta) -> 1, as beta -> infinity. Under these hypothesis we will show that 1/beta (u(lambda,beta) - P(beta A)/1-lambda) converges uniformly to the above V, as beta -> infinity. The parameter beta represents the inverse of temperature in Statistical Mechanics and beta -> infinity means that we are considering that the temperature goes to zero. Under these conditions we get selection of subaction when beta -> infinity.
机译:考虑作用于S-1的T(x)= dx(mod 1),一个Lipschitz势A:S-1-> R,0 R满足b(lambda)(x)= max(T(y)= x){lambda b(lambda)(y)+ A(y)}。我们将证明,当lambda-> 1时,函数b(lambda) -m(A)/ 1-lambda均匀收敛到校准子作用V(x)= max(mu是M的元素)积分S(y,x)d mu(y),其中S是Mane势,M是在Aubry集上具有支持的不变概率集,并且m(A)= sup(mu是M)整数Ad mu的元素。对于beta> 0且lambda是(0,1)的元素,存在一个方程的唯一不动点u(lambda,beta):S-1-> R e(u lambda,beta(x))= Sigma(T(y)())(= x)e(beta A(y) + lambda u lambda,beta(y))。众所周知,作为lambda-> 1族,e([u lambda,β-supulambda,β)均匀收敛于与βA相关的Ruelle算子的主要特征函数phiβ。我们认为lambda = lambda( beta),beta(1-lambdaβ)-> + infinity和lambdaβ-> 1,即beta-> infinity。在这些假设下,我们将显示1 / beta(u(lambda,beta)-P(beta A)/ 1-lambda)均匀收敛于上述V,即beta->无穷大。参数beta表示统计力学中的温度的倒数,而beta-> infinity表示我们正在考虑温度变为零。在这些条件下,当beta-> infinity时,我们可以选择子动作。

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