2021
DOI: 10.1093/imrn/rnab318
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Improved Versions of Some Furstenberg Type Slicing Theorems for Self-Affine Carpets

Abstract: Let $F$ be a Bedford–McMullen carpet defined by independent integer exponents. We prove that for every line $\ell \subseteq \mathbb{R}^2$ not parallel to the major axes, $$\begin{align*} & \dim_H (\ell \cap F) \leq \max \left\lbrace 0,\, \frac{\dim_H F}{\dim^* F} \cdot (\dim^* F-1) \right\rbrace\end{align*}$$and $$\begin{align*} & \dim_P (\ell \cap F) \leq \max \left\lbrace 0,\, \frac{\dim_P F}{\dim^* F} \cdot (\dim^* F-1) \right\rbrace,\end{align*}$$where $\dim ^*$ is Furstenberg’s star dimension (max… Show more

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Cited by 2 publications
(18 citation statements)
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“…The general lower bound of [2,14] is a concave function between .0; 0/ and .1; dim B ƒ/, which enables to construct an example which shows that dim  ƒ is not convex in general; see Fig- In Figure 4.1, the (orange) plot depicting the upper bound comes from Theorem 1.2, while the (blue) plot depicting the lower bound comes from a combination of results in [2,14,22]. The ratio log n m has an important role in projection and slicing results about Bedford-McMullen carpets [1,15] and the Assouad spectrum has a phase transition here [18]. These together with Claim 2.2 strongly suggest to us that dim  ƒ may have a phase transition at log n m. Can dim  ƒ have additional phase transitions at other integer powers of log n m?…”
Section: Further Discussionmentioning
confidence: 99%
“…The general lower bound of [2,14] is a concave function between .0; 0/ and .1; dim B ƒ/, which enables to construct an example which shows that dim  ƒ is not convex in general; see Fig- In Figure 4.1, the (orange) plot depicting the upper bound comes from Theorem 1.2, while the (blue) plot depicting the lower bound comes from a combination of results in [2,14,22]. The ratio log n m has an important role in projection and slicing results about Bedford-McMullen carpets [1,15] and the Assouad spectrum has a phase transition here [18]. These together with Claim 2.2 strongly suggest to us that dim  ƒ may have a phase transition at log n m. Can dim  ƒ have additional phase transitions at other integer powers of log n m?…”
Section: Further Discussionmentioning
confidence: 99%
“…Let 𝑐 > 0 be an absolute constant to be determined a little later. We apply Proposition 2.1 at scale Δ with parameters 𝜖 = 𝜂 2 and 𝐴 ∶= 𝑐𝑆 and to the families {𝐵 𝑝 ∶ 𝑝 ∈  Δ } and {𝕋 𝑇 ∶ 𝑇 ∈  Δ } (recall that ( Δ ,  Δ ) is defined using these balls and ordinary tubes). The proposition requires 𝐴 ∈ [Δ −𝜂 2 , Δ −1 ], and this is satisfied because 𝐴 ⩽ 𝑆 = 𝛿 −𝜂 ⩽ Δ −1 .…”
Section: A New Incidence Estimatementioning
confidence: 99%
“…Theorem 5.2. For every 𝑡 ∈ (1,2] and 𝑠 ∈ [𝑡 − 1, 1 3 (2𝑡 − 1)] there exists a compact set  ⊂ (2, 1) consisting of non-vertical lines, and with the following properties.…”
Section: Continuous Sharpness Examplesmentioning
confidence: 99%
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