A formula for the Entropy of the Convolution of Gibbs probabilities on the circle
Abstract
Consider the transformation T:S1 S1, such that T(x)=2\, x (mod 1), and where S1 is the unitary circle. Suppose J:S1 R is Holder continuous and positive, and moreover that, for any y∈ S1, we have that Σx\,\,such that\,\,\, T(x)= y \, J(x)=1. We say that is a Gibbs probability for the Holder continuous potential J, if L J* \,()= , where L J is the Ruelle operator for J. We call J the Jacobian of . Suppose =μ1*μ2 is the convolution of two Gibbs probabilities μ1 and μ2 associated, respectively, to J1 and J2. We show that is also Gibbs and its Jacobian J is given by J(u) = ∫ J1(u-x) d μ2(x) In this case, the entropy h() is given by the expression h() = - ∫\,[\,\,∫\, \,(\,∫ J1(r+s-x) d μ2(x)\,) \, d μ2(r)\,\, ]\,\,d μ1 (s). For a fixed μ2 we consider differentiable variations μ1t, t ∈ (-ε,ε), of μ1 on the Banach manifold of Gibbs probabilities, where μ10=μ1, and we estimate the derivative of the entropy h(μ1t * μ2) at t=0. We also present an expression for the Jacobian of the convolution of a Gibbs probability with the invariant probability with support on a periodic orbit of period two. This expression is based on the Jacobian of and two Radon-Nidodym derivatives.
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