Abstract

A central role in the variational principle of the measure preserving transformations is played by the topological pressure. We introduce subadditive pre-image topological pressure and pre-image measure-theoretic entropy properly for the random bundle transformations on a class of measurable subsets. On the basis of these notions, we are able to complete the subadditive pre-image variational principle under relatively weak conditions for the bundle random dynamical systems.

Highlights

  • The topological pressure and variational principle play an important role in statistical mechanics, ergodic theory, and dynamical systems [1,2,3,4,5,6,7,8]

  • We present the notion of subadditive pre-image topological pressure Ppre ( T, Φ) for continuous random dynamical systems

  • We set up a variational principle for subadditive pre-image topological pressure for continuous bundle random dynamical systems

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Summary

Introduction

The topological pressure and variational principle play an important role in statistical mechanics, ergodic theory, and dynamical systems [1,2,3,4,5,6,7,8]. Ppre ( T, f ) = sup{ hpre, μ ( T ) + μ( f ) : μ ∈ M( T )}, where hpre, μ ( T ) is the pre-image measure-theoretic entropy, M( T ) is the set of T-invariant measures on the compact metric space X. We present the notion of subadditive pre-image topological pressure Ppre ( T, Φ) for continuous random dynamical systems. As for the case of −∞, the subadditive pre-image topological pressure is tightly relative to the limit function Φ∗ (μ), which is −∞ for all invariant measure μ. The pre-image measure-theoretic (relativized) entropy hpre, μ ( T ) of the RDS T with respect to μ ∈ M1P (E , T ) is defined by the formula hpre, μ ( T ) = sup hpre, μ ( T, Q),. We will use these results directly and not give these proofs since it seems that there is no different from the arguments in [30] except changing the symbols and restricting to the measurable subset E

Subadditive Pre-Image Topological Pressure
Subadditive Pre-Image Variational Principle
Conclusions
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