2508.04083
Connectedness of independence attractors of graphs with independence number three
Moumita Manna, Tarakanta Nayak
wrongmedium confidenceCounterexample detected
- Category
- math.DS
- Journal tier
- Strong Field
- Processed
- Sep 28, 2025, 12:57 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper defines the independence attractor as A(G) = lim_m Roots(IG^m), with IG^m(z) = P_G^m(z) + 1 and hence Roots(IG^m) = {z : P_G^m(z) = −1} (Definition 2.1 and (2.1) ). In the unicritical 3-vertex case a1=3, P(z) = (1+z)^3−1, so P^m(z) = (1+z)^{3^m}−1 and Roots(IG^m) = {−1} for all m; the Hausdorff limit is therefore {−1}. However, the paper asserts (Theorem 1.2) that A(G) equals {−1} ∪ {|z+1|=1} for a1=3, appealing to Theorem 1.5 which claims that, in an exceptional family (including a1=3), A(G) is the disjoint union of J(P_G) and ⋃_{k≥1} Roots(IG^k) . This contradicts the literal limit: in the a1=3 case, ⋃_{k≥1} Roots(IG^k) = {−1}, so the Hausdorff limit cannot suddenly include the circle. The model flags exactly this definitional inconsistency and shows that the intended classification holds if one instead takes A0(G) := lim_m Roots(IG^m−1) = lim_m Roots(P_G^m), i.e., preimages of 0, which equals J(P_G) by standard Fatou–Julia theory. Apart from this definitional error, the paper’s connectivity sub-classification of J(P) along the curves a2^2 = 3a1a3, 4a3(a1−1), 4a1a3 and the finer thresholds matches the model’s dynamics-based derivations (e.g., Lemma 3.7 and Lemma 3.8) .
Referee report (LaTeX)
\textbf{Recommendation:} major revisions \textbf{Journal Tier:} strong field \textbf{Justification:} The results on the dynamical classification relative to the parameters (a1,a2,a3) are valuable and appear correct when interpreted as statements about the Julia set of the reduced independence polynomial. However, the paper's definition of independence attractor as a Hausdorff limit of Roots(IG\^m) conflicts with its assertion that in the exceptional family (including a1=3) the attractor contains the Julia set. This inconsistency must be resolved—either by redefining the attractor so that it always includes J(P\_G) together with an explanation of its equivalence in the non-exceptional cases, or by amending the exceptional-case claims.