- The paper extends geometric partial attraction and merge theorems for maxima of Bernoulli-convolution AR(1) processes to every β∈(0,1), despite unresolved singularity and absolute-continuity properties.
- It represents the stationary distribution through a log-periodic function on a key subinterval and uses extension and reflection methods to characterize the full distribution, while showing that periodicity may fail globally.
- The dependent AR(1) process converges to a Weibull-type max-semistable law with extremal index p, revealing clustering of extremes and a loss of effective independent observations that does not depend on β.
Setting and motivation
The paper studies the simple autoregressive process Xk+1=βXk+εk+1, where the innovations εk take the values $0$ and 1−β with probabilities p and q=1−p, for β∈(0,1). The stationary solution Xk=∑j≥0βjεk−j is, up to an affine transformation, a Bernoulli convolution ∑j≥0βjZj with P(Zj=−1)=p, εk0. Prior work [(2608.14155)'s predecessor, Sterk (2025)] established max-semistable extremal behavior for εk1, where the support is a Cantor-like set. The contribution here is to extend this to the full range εk2, where the stationary distribution may be absolutely continuous or singular depending on delicate arithmetic properties of εk3 (Pisot and Garsia numbers, Solomyak's almost-sure absolute continuity result). The paper deliberately does not resolve the singularity/absolute-continuity dichotomy; instead it derives a structural representation of the distribution function that suffices for extreme value theory regardless of that dichotomy.
Structural representation of the stationary distribution
The stationary distribution function εk4 satisfies the refinement equation
εk5
with support in εk6. A first result extends uniqueness of the continuous solution of this functional equation from εk7 to all εk8, via a contraction argument on the sup-norm that works for the entire parameter range. A symmetry relation εk9 is also recorded.
The key structural result is a partial extension of the log-periodic representation known for $0$0: for $0$1 one has
$0$2
with $0$3 continuous and $0$4-periodic. Crucially, the representation holds only on the left part of the support. Numerical approximations for the golden-ratio parameter indicate that the periodicity of $0$5 genuinely breaks down beyond $0$6, so the full analogue of the $0$7 result is false in general. The paper then offers two devices to characterize $0$8 on the whole interval $0$9 in terms of 1−β0: an extension method, which iteratively applies the functional equation outward from 1−β1 and whose critical steps occur exactly at Pisot numbers (e.g., 1−β2 and the plastic number 1−β3), and a reflection method based on the symmetry relation, which closes the gap entirely when 1−β4. These methods yield structural insight but, as the authors concede, do not produce explicit closed forms for 1−β5 or 1−β6.
Two worked examples illustrate when the periodic function degenerates to a constant, which would yield a max-stable (rather than merely max-semistable) limit. For 1−β7, 1−β8 (a Garsia parameter), the extension method rigorously reconstructs the known piecewise-quadratic distribution with a tent-like density, confirming a constant 1−β9 and hence a max-stable limit. For p0 with p1 the extension is carried out for p2, but the authors explicitly state it remains unclear whether the constant-p3 ansatz actually satisfies the functional equation; only numerical evidence is offered.
Domain of geometric partial attraction
Since extremes of an i.i.d. sample from p4 are governed by the behavior of p5 near p6, and by the symmetry relation near p7, the log-periodic representation of p8 suffices. The main i.i.d. result states that with p9, q=1−p0, and the geometrically growing subsequence q=1−p1,
q=1−p2
a max-semistable law of Weibull type with parameters q=1−p3 and q=1−p4. The proof is a direct computation exploiting the periodicity of q=1−p5, avoiding general domain-of-attraction criteria. The result thus extends the geometric-partial-attraction property from q=1−p6 to the full range q=1−p7. The authors note the theorem does not exclude a constant q=1−p8 (max-stable limit), and cite numerical evidence in Solomyak's notes for the case q=1−p9.
Merge theorems
Convergence along the single subsequence β∈(0,1)0 is refined into a merge theorem, valid for all β∈(0,1)1. Writing β∈(0,1)2 with β∈(0,1)3 and using the modified normalization β∈(0,1)4, the i.i.d. merge theorem asserts uniform convergence
β∈(0,1)5
where β∈(0,1)6 is the max-semistable limit. The proof is a simplification of Megyesi's general argument, made possible by continuity of β∈(0,1)7, and proceeds by a subsequence argument: along subsequences with β∈(0,1)8, pointwise convergence to β∈(0,1)9 holds, uniformity on compacts follows, and a compactness argument on the relatively compact sequence Xk=∑j≥0βjεk−j0 closes the proof. A modified normalization Xk=∑j≥0βjεk−j1 additionally makes the limit independent of the accumulation point of Xk=∑j≥0βjεk−j2, using the periodicity of Xk=∑j≥0βjεk−j3.
The corresponding result for the stationary Xk=∑j≥0βjεk−j4 process is the paper's main theorem. The proof follows the blocking technique of Chernick and of Glavaš–Mladenović–Samorodnitsky: the index set is partitioned into long blocks separated by vanishing gaps, and the four error terms (boundary loss, gap loss, asymptotic independence across blocks, and endpoint mismatch) are shown to vanish. The technically demanding part is establishing asymptotic independence between disjoint blocks; this is handled through a careful regular-conditional-probability computation exploiting the decomposition Xk=∑j≥0βjεk−j5 with Xk=∑j≥0βjεk−j6 independent of the past and bounded by Xk=∑j≥0βjεk−j7. The outcome is the Xk=∑j≥0βjεk−j8 merge theorem
Xk=∑j≥0βjεk−j9
and, along ∑j≥0βjZj0, uniform convergence to ∑j≥0βjZj1. Comparing with the i.i.d. case, the process has extremal index ∑j≥0βjZj2, interpretable as loss of i.i.d. degrees of freedom, the reciprocal expected cluster size, or the recurrence rate near unstable fixed points of associated dynamical systems. Notably, the extremal index is independent of ∑j≥0βjZj3.
Connections with dynamical systems
Two dynamical interpretations of ∑j≥0βjZj4 are given. First, the skew-product map ∑j≥0βjZj5 on ∑j≥0βjZj6, which for ∑j≥0βjZj7 is topologically conjugate to the generalized baker's transformation of Alexander–Yorke, preserves the product-type measure built from ∑j≥0βjZj8 in the ∑j≥0βjZj9-direction and Lebesgue measure in the driving coordinate; invariance is verified directly on generating rectangles via the functional equation. Since the driving map has exponential decay of correlations, the P(Zj=−1)=p0-projection of P(Zj=−1)=p1-orbits serves as a deterministic counterpart of the P(Zj=−1)=p2 process, linking the results to extreme value laws for deterministic dynamical systems. Second, in the random-iteration framework of Mitrea–Sterk, the probability P(Zj=−1)=p3 that random compositions of two expanding maps diverge satisfies the same functional equation and boundary conditions as P(Zj=−1)=p4 for P(Zj=−1)=p5 and P(Zj=−1)=p6; by the uniqueness lemma the two functions coincide for P(Zj=−1)=p7. This identification rests on the uniqueness result and therefore extends verbatim to all P(Zj=−1)=p8.
Limitations and open questions
The paper is explicit about several boundaries of its results. The log-periodic representation is established only on P(Zj=−1)=p9, and numerical evidence suggests it does not extend further in general; the extension and reflection methods characterize εk00 implicitly but do not yield explicit formulas for εk01. Whether the max-semistable limit is genuinely non-max-stable for most parameters — equivalently, whether εk02 is non-constant — is unresolved; the constant case is proven only for εk03, εk04, and conjectured numerically for εk05, εk06, where the functional-equation verification is left incomplete. The question of which εk07 yield singular versus absolutely continuous stationary distributions is inherited from the Bernoulli convolution literature and untouched here. Finally, whether the deterministic skew-product εk08 admits an extreme value law with the same limit and extremal index εk09 is raised by the analogy but not proven.
Conclusion
The paper completes the max-semistable extreme value analysis of the Bernoulli-convolution AR(1) process across the full parameter range εk10. Its two central contributions are a partial log-periodic representation of the stationary distribution function that suffices for extremal analysis despite holding only on a subinterval, and merge theorems — for both i.i.d. sequences and the dependent εk11 process — establishing uniform convergence of normalized maxima to powers of a Weibull-type max-semistable law with extremal index εk12. The results are robust to the singular/absolutely-continuous dichotomy of the underlying Bernoulli convolution, while the identification of the exact limit law (semistable versus stable) remains tied to open arithmetic questions about the parameter εk13.