mlsanityData to 14 Oct 2026

Entropy, Pressure and Duality for Gibbs plans in Ergodic Transport

arXiv 1308.6514 ↗First posted 29 Aug 2013math.DS cond-mat.stat-mech math-phcited by 1

Not on the map. Why?

Abstract (arXiv)

Let X be a finite set and Omega=1,...,d^mathbbN be the Bernoulli space. Denote by σ the shift map acting on Omega. For a fixed probability μ on X with supp(μ)=X, define Pi(μ,σ) as the set of all Borel probabilities π ∈ P(X× Omega) such that the x-marginal of π is μ and the y-marginal of π is σ-invariant. We consider a fixed Lipschitz cost function c: X × Omega → ℝ and an associated Ruelle operator. We introduce the concept of Gibbs plan, which is a probability on X × Omega. Moreover, we define entropy, pressure and equilibrium plans. The study of equilibrium plans can be seen as a generalization of the optimal cost problem where the concept of entropy is introduced. We show that an equilibrium plan is a Gibbs plan. Our main result is a Kantorovich duality Theorem on this setting. The pressure plays an important role in the establishment of the notion of admissible pair. Finally, given a parameter β, which plays the role of the inverse of temperature, we consider equilibrium plans for β c and its limit π_∞, when β → ∞, which is also known as ground state. We compare this with other previous results on Ergodic Transport in temperature zero.

Key facts. Cited by 1 paper in the map (data through 14 Oct 2026). First posted on arXiv 29 Aug 2013.

Builds on

No reference list yet.

Built on by

Cited by year

Citing papers per year: 2021: 1.

1 paper.