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Transcendental Julia sets of minimal Hausdorff dimension

Published online by Cambridge University Press:  06 January 2025

JACK BURKART*
Affiliation:
Bard College at Simon’s Rock, 84 Alford Road, Great Barrington, MA 01230, USA
KIRILL LAZEBNIK
Affiliation:
Department of Mathematical Sciences, The University of Texas at Dallas, 800 W. Campbell Road, Richardson, TX 75080, USA (e-mail: Kirill.Lazebnik@UTDallas.edu)
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Abstract

We show the existence of transcendental entire functions $f: \mathbb {C} \rightarrow \mathbb {C}$ with Hausdorff-dimension $1$ Julia sets, such that every Fatou component of f has infinite inner connectivity. We also show that there exist singleton complementary components of any Fatou component of f, answering a question of Rippon and Stallard [Eremenko points and the structure of the escaping set. Trans. Amer. Math. Soc. 372(5) (2019), 3083–3111]. Our proof relies on a quasiconformal-surgery approach developed by Burkart and Lazebnik [Interpolation of power mappings. Rev. Mat. Iberoam. 39(3) (2023), 1181–1200].

Information

Type
Original Article
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 Panels (a) and (b) illustrate the concept of infinite outer-connectivity and infinite inner-connectivity, respectively. Panels (a) and (b) also accurately describe the topology of the m.c.w.d.s in [Bis18] and Theorem 1.1, respectively. As seen, the structure in panel (b) is more intricate.

Figure 1

Figure 2 Definition of $A_k$, $B_k$ for all $k\in \mathbb {Z}$. The annuli $A_k$ are shaded light gray and the $B_k$ are white. Also shown are $V_1\subset A_1$ and the ‘petals’ $P_j\subset A_1$ (in dark gray).

Figure 2

Table 1 The values of $M_k$, $c_k$, and $r_k$ for small values of k. The sequence $M_k$ increases exponentially and $r_k$ increases super-exponentially, while $c_k$ decays super-exponentially.

Figure 3

Figure 3 A visualization of $A_k$ and $B_k$ viewed on the cylinder. The annuli $A_k$ have constant modulus, and the annulus $B_k$ have very large and increasing moduli.

Figure 4

Figure 4 $f_N$ maps the annulus $B_k$ into the annulus $B_{k+1}$. The picture is not to scale; in reality, the modulus of $B_{k+1}$ is much larger than the modulus of $f_N(B_k)$.

Figure 5

Figure 5 A schematic for Definition 5.4 and Lemma 5.5. The critical points for $q_N$ lie on the circle $|z| = ({r_N}/{c_NM_N})^{{1}/{M_N-1}}$, and the associated critical values lie in an annulus contained in V, illustrated in gray. So, U contains the critical points of $q_N$, and it will also be verified that $U \subset D$.

Figure 6

Figure 6 Illustration of Definition 5.8 of the families $\Gamma _n$.

Figure 7

Figure 7 Illustration of Definition 6.2 of the petals $P_k$. The annuli $B_{k-1}$, $B_k$ are in white, the annulus $A_k$ is in light gray, and the annulus $V_k$ and petals $P_k$ are in dark gray.

Figure 8

Figure 8 Illustration of Definition 7.1 of $A_k$, $B_k$ for negative k. Each connected component of $A_0$ maps conformally onto $A_1$; therefore, each connected component of $A_0$ contains $2^N$ many connected components of $A_{-1}$. The picture repeats itself as we zoom in. The set $B_0$ is the region between the outer boundaries of the components of $A_0$ and the inner boundary of $A_1$.

Figure 9

Figure 9 Illustration of the covering $\mathcal {C}_1$ and the notation $W_k^n$ for elements of $\mathcal {C}_1$ (see Notation 8.3). The elements of $\mathcal {C}_m$ for $m>1$ are obtained by essentially placing a scaled-down copy of $\mathcal {C}_{m-1}$ in each annulus in the covering $\mathcal {C}_{m-1}$.

Figure 10

Figure 10 An illustration of components of the form $\widehat W^{n+q}_{k+q-1} \in \widehat {\mathcal {C}}_{m+1}$ contained inside of some $W^n_k \in \mathcal {C}_m$ for $q=1,2,$ and $3$. The component $W^n_k$ is bounded by the innermost and outermost circle.

Figure 11

Figure 11 A schematic for the statement of Lemma 9.3.

Figure 12

Figure 12 A schematic for the proof of Lemma 9.4.

Figure 13

Figure 13 A schematic for the proof of Lemma 9.8 in the key step of $m =1$ and $n=0$. In this case, $\gamma _0$ and $f_N(\gamma _1)$ are circles, and $(Df_N):T_z\mathbb {C} \rightarrow T_{f_N(z)}\mathbb {C}$ maps the outward pointing normal $\nu _1(z)$ to $\gamma _1$ to an outward pointing normal $(Df_N)_z(\nu _1(z))$ of the circle $f_N(\gamma _1)$. This allows us to apply Lemma 9.4 to estimate the angle between $(Df_N)_z(\nu _1(z))$ and $(Df_N)_z(\nu _0(z))$, which coincides with the angle between $\nu _1(z)$ and $\nu _0(z)$.

Figure 14

Figure 14 A schematic for the proof of Corollary 9.9. If some ray R passed through $\gamma $ at more than one point, there is a ray $R'$ tangent to $\gamma $ at some other point z. If C is the circle centered at the origin passing through z, the normal vectors $\nu _{\gamma }(z)$ and $\nu _C(z)$ make an angle of $\pi /2$ with each other.

Figure 15

Figure 15 Illustration of a brief sketch of the curves $\gamma _k^m$ for $0\leq k \leq m$.