Definition:Ruelle-Perron-Frobenius Operator/One-Sided Shift Space of Finite Type
Jump to navigation
Jump to search
![]() | This article is complete as far as it goes, but it could do with expansion. In particular: Parent page You can help $\mathsf{Pr} \infty \mathsf{fWiki}$ by adding this information. To discuss this page in more detail, feel free to use the talk page. When this work has been completed, you may remove this instance of {{Expand}} from the code.If you would welcome a second opinion as to whether your work is correct, add a call to {{Proofread}} the page. |
Definition
Let $\struct {X_\mathbf A ^+, \sigma}$ be a one-sided shift of finite type.
Let $\map C {X _\mathbf A ^+, \C}$ be the continuous mapping space.
Let $F_\theta^+$ be the space of Lipschitz functions on $X_\mathbf A ^+$.
Let $B$ be either $\map C {X _\mathbf A ^+, \C}$ or $F_\theta^+$.
Let $f \in B$.
The Ruelle-Perron-Frobenius operator $\LL_f : B \to B$ is defined as:
- $\ds \forall g \in B : \map {\paren {\LL_f g} } x := \sum_{y \mathop \in \map {\sigma^{-1} } x} e^{\map f y} \map g y$
where $\map {\sigma^{-1} } x$ denotes the preimage of $x$ under $\sigma$:
- $\map {\sigma^{-1} } x = \set {\sequence {i, x_0, x_1, \ldots} : \map {\mathbf A} {i, x_0} = 1}$
Also known as
This is also called:
- the transfer operator
- the Ruelle operator.
Also see
Source of Name
This entry was named for David Pierre Ruelle, Oskar Perron and Ferdinand Georg Frobenius.
Sources
- 1990: William Parry and Mark Pollicott: Zeta Functions and the Periodic Orbit Structure of Hyperbolic Dynamics: Chapter $2$: The Ruelle Operator