2011
DOI: 10.1016/j.jmaa.2011.01.046
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On the pointwise densities of the Cantor measure

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Cited by 6 publications
(6 citation statements)
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“…In particular, d * = 2d * , independent of ρ. Wang, Wu and Xiong [25] later extended theorem 1.1 to the interval 0 < ρ ρ * , where ρ * ≈ 0.351 811 satisfies (1 − ρ * ) s(ρ * ) = 3/4. However, they showed that for ρ > ρ * , the formula for the upper density changes.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, d * = 2d * , independent of ρ. Wang, Wu and Xiong [25] later extended theorem 1.1 to the interval 0 < ρ ρ * , where ρ * ≈ 0.351 811 satisfies (1 − ρ * ) s(ρ * ) = 3/4. However, they showed that for ρ > ρ * , the formula for the upper density changes.…”
Section: Introductionmentioning
confidence: 99%
“…The study of densities for a self-similar measure attracted a lot of attention in the literature (see [3,4,7,17,18,19] and the references therein). When N = 2 and ρ ∈ (0, 1/3], Feng et al [8] explicitly calculated the pointwise densities Θ s * (µ, x) and Θ * s (µ, x) for any x ∈ E. The upper bound 1/3 for ρ was later improved to ( √ 3 − 1)/2 by Wang et al [20]. Motivated by their work, Li and Yao [14] determined the pointwise densities of the self-similar measure for non-homogeneous self-similar IFSs.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, d * = 2d * , independent of ρ. Wang et al [20] later extended Theorem 1.1 to the interval 0 < ρ ≤ ρ * , where ρ * ≈ .351811 satisfies (1 − ρ * ) s(ρ * ) = 3/4.…”
Section: Introductionmentioning
confidence: 99%
“…A first observation is that Γ ⊆ C, since lim inf n→∞ T n (x) ∈ C and lim inf n→∞ T n (1−x) ∈ C for every x ∈ C. In [20,Theorem 1.3] Wang et al initiated the study of Γ, but their characterization was rather abstract. By connecting the quantities τ (x) with the theory of unique non-integer base exansions, we are able to give a much more explicit description of Γ here.…”
Section: Introductionmentioning
confidence: 99%