2101.02546
Thermodynamic Formalism for Generalized Countable Markov Shifts
Thiago Costa Raszeja
correctmedium confidence
- Category
- Not specified
- Journal tier
- Specialist/Solid
- Processed
- Sep 28, 2025, 12:55 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper’s Theorem (for the generalized renewal shift with F(x)=log(x0)−log(x0+1)) states: for every β>0 there is a unique eigenmeasure for λβ=e^{PG(βF)}, with a critical βc determined by ζ(βc)=2; if β>βc the eigenmeasure is supported on YA, and if β≤βc it is supported on ΣA. The thesis proves this by combining a renewal computation of return weights Z*_n=(n+1)^{-β}, Sarig’s discriminant/recurrence theory to get the phase transition, and Denker–Yuri’s IFS “pressure at a point” to guarantee existence/uniqueness on XA; it also gives explicit cylinder-mass formulas and shows PG(βF)=0 for β≥βc (eigenvalue 1) (see the statement and proof around Theorem 5.54 and Example 5, including (5.64)–(5.70) and the ζ(β)=2 threshold) . The candidate solution reaches the same conclusions by a standard renewal generating-function argument for pressure/λβ and by appealing to transient Ruelle theory/Martin boundary for β>βc. While the model’s reasoning is correct for this example and matches the paper’s conclusions (including the exact threshold ζ(βc)=2 and the support switch), some steps (e.g., uniqueness via Martin boundary and applicability beyond locally compact ΣA) are not the route used in the paper and would need additional justification. Net: same result, different proof routes; both are correct.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions
\textbf{Journal Tier:} specialist/solid
\textbf{Justification:}
The theorem is stated and proved cleanly, giving a complete description of the length-type phase transition for the renewal model on XA: existence/uniqueness for all β>0, exact threshold ζ(βc)=2, and a support switch between ΣA and YA. The route via IFS pressure at a point and explicit cylinder computations is convincing and self-contained. A few editorial additions (briefly recalling why pressure at a point coincides with Gurevich pressure here, highlighting explicit formulas) would further aid readers.