English

Fibre stability for dominated self-affine sets

Dynamical Systems 2024-12-10 v1 Classical Analysis and ODEs Metric Geometry

Abstract

Let KK be a planar self-affine set. Assuming a weak domination condition on the matrix parts, we prove for all backward Furstenberg directions VV that maxETan(K)maxxπV(E)dimH(πV1(x)E)=dimAKdimAπV(K).\max_{E\in\operatorname{Tan}(K)} \max_{x\in \pi_{V^\bot}(E)} \operatorname{dim_H} (\pi_{V^\bot}^{-1}(x)\cap E) = \operatorname{dim_A} K - \operatorname{dim_A} \pi_{V^\bot}(K). Here, Tan(K)\operatorname{Tan}(K) denotes the space of weak tangents of KK. Unlike previous work on this topic, we require no separation or irreducibility assumptions. However, if in addition the strong separation condition holds, then there exists a VXFV\in X_F so that maxxπV(K)dimH(πV1(x)K)=dimAKdimAπV(K).\max_{x\in \pi_{V^\bot}(K)} \operatorname{dim_H} (\pi_{V^\bot}^{-1}(x)\cap K) = \operatorname{dim_A} K - \operatorname{dim_A} \pi_{V^\bot}(K). Our key innovation is an amplification result for slices of weak tangents via pigeonholing arguments.

Cite

@article{arxiv.2412.06579,
  title  = {Fibre stability for dominated self-affine sets},
  author = {Roope Anttila and Alex Rutar},
  journal= {arXiv preprint arXiv:2412.06579},
  year   = {2024}
}

Comments

35 pages + 3 page appendix, 1 figure

R2 v1 2026-06-28T20:28:01.337Z