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Given ρ ∈ (0, 1/3], let μ be the Cantor measure satisfying μ = 1 2 μ f 0 − 1 + 1 2 μ f 1 − 1 , where f i (x) = ρx + i(1 − ρ) for i = 0, 1. The support of μ is a Cantor set C generated by the iterated function system {f 0, f 1}. Continuing the work of Feng et al (2000) on the pointwise lower and upper densities Θ * s ( μ , x ) = lim inf r → 0 μ ( B ( x , r ) ) ( 2 r ) s , Θ * s ( μ , x ) = lim sup r → 0 μ ( B ( x , r ) ) ( 2 r ) s , where s = −log 2/log ρ is the Hausdorff dimension of C, we give a complete description of the sets D * and D* consisting of all possible values of the lower and upper densities, respectively. We show that both sets contain infinitely many isolated and infinitely many accumulation points, and they have the same Hausdorff dimension as the Cantor set C. Furthermore, we compute the Hausdorff dimension of the level sets of the lower and upper densities. Our method consists in formulating an equivalent ‘dyadic’ version of the problem involving the doubling map on [0, 1), which we solve by using known results on the entropy of a certain open dynamical system and the notion of tuning.
Given ρ ∈ (0, 1/3], let μ be the Cantor measure satisfying μ = 1 2 μ f 0 − 1 + 1 2 μ f 1 − 1 , where f i (x) = ρx + i(1 − ρ) for i = 0, 1. The support of μ is a Cantor set C generated by the iterated function system {f 0, f 1}. Continuing the work of Feng et al (2000) on the pointwise lower and upper densities Θ * s ( μ , x ) = lim inf r → 0 μ ( B ( x , r ) ) ( 2 r ) s , Θ * s ( μ , x ) = lim sup r → 0 μ ( B ( x , r ) ) ( 2 r ) s , where s = −log 2/log ρ is the Hausdorff dimension of C, we give a complete description of the sets D * and D* consisting of all possible values of the lower and upper densities, respectively. We show that both sets contain infinitely many isolated and infinitely many accumulation points, and they have the same Hausdorff dimension as the Cantor set C. Furthermore, we compute the Hausdorff dimension of the level sets of the lower and upper densities. Our method consists in formulating an equivalent ‘dyadic’ version of the problem involving the doubling map on [0, 1), which we solve by using known results on the entropy of a certain open dynamical system and the notion of tuning.
Let N ≥ 2 and ρ ∈ (0, 1/N 2 ]. The homogenous Cantor set E is the self-similar set generated by the iterated function systemLet s = dimH E be the Hausdorff dimension of E, and let µ = H s |E be the s-dimensional Hausdorff measure restricted to E. In this paper we describe, for each x ∈ E, the pointwise lower s-density Θ s * (µ, x) and upper s-density Θ * s (µ, x) of µ at x. This extends some early results of Feng et al. (2000). Furthermore, we determine two critical values ac and bc for the sets E * (a) = {x ∈ E : Θ s * (µ, x) ≥ a} and E * (b) = {x ∈ E : Θ * s (µ, x) ≤ b} respectively, such that dimH E * (a) > 0 if and only if a < ac, and that dimH E * (b) > 0 if and only if b > bc. We emphasize that both values ac and bc are related to the Thue-Morse type sequences, and our strategy to find them relies on ideas from open dynamics and techniques from combinatorics on words.
Given ρ ∈ (0, 1/3], let µ be the Cantor measure satisfying µ = 1 2 µf −1 0 + 1 2 µf −1 1 , where fi(x) = ρx + i(1 − ρ) for i = 0, 1. The support of µ is a Cantor set C generated by the iterated function system {f0, f1}. Continuing the work of Feng et al. (2000) on the pointwise lower and upper densitieswhere s = − log 2/ log ρ is the Hausdorff dimension of C, we give a complete description of the sets D * and D * consisting of all possible values of the lower and upper densities, respectively. We show that both sets contain infinitely many isolated and infinitely many accumulation points, and they have the same Hausdorff dimension as the Cantor set C. Furthermore, we compute the Hausdorff dimension of the level sets of the lower and upper densities. Our proofs are based on recent progress on unique non-integer base expansions and ideas from open dynamical systems.
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