A Self-Similar Dendrite with One-Point Intersection and Infinite Post-Critical Set
Prabhjot Singh, Andrey Tetenov

TL;DR
This paper constructs a specific self-similar dendrite in the plane with a one-point intersection property and a dense, countable post-critical set, revealing complex topological and dynamical features.
Contribution
It introduces a novel example of a self-similar system with unique intersection and post-critical set properties not previously documented.
Findings
The attractor is a plane dendrite containing [0,1].
The post-critical set is countable and dense in a Cantor set.
The system exhibits one point intersection property.
Abstract
We build an example of a system of similarities in whose attractor is a plane dendrite which satisfies one point intersection property, while the post-critical set of the system is a countable set whose natural projection to is dense in the middle-third Cantor set.
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Taxonomy
TopicsMathematical Dynamics and Fractals · Cellular Automata and Applications
A Self-Similar Dendrite with One-Point Intersection and
Infinite Post-Critical Set.
Prabhjot Singh
Andrey Tetenov111Supported by Russian Foundation of Basic Research project 16-01-00414
Abstract
We build an example of a system of similarities in whose attractor is a plane dendrite which satisfies one point intersection property, while the post-critical set of the system is a countable set whose natural projection to is dense in the middle-third Cantor set.
MSC classification: 28A80
1 Introduction
Let be a system of contraction maps in . A non-empty compact set satisfying is called invariant set, or attractor, of the system . The uniqueness and existence of the attractor is provided by Hutchinson’s Theorem [3].
Let , be the set of all finite -tuples and be the index space and be the address map.
A system satisfies open set condition(OSC) if there is nonempty open such that and = for any [3, 5]. We say that the system satisfies one point intersection property [1] if for any , .
Let be the union of all , . The post-critical set of the system is the set of all such that for some , . In other words, , where the map is defined by .
A system is called post-critically finite(pcf) [4] if its post-critical set is finite. This obviously implies finite intersection property.
Our aim is to show that the converse need not be true even in the case of plane dendrites. We construct an example of pcf system , whose attractor is a dendrite , satisfying one point intersection property.
So we prove the following
Theorem 1**.**
There is a system in , whose attractor is a dendrite, which satisfies OSC and 1-point intersection property and has infinite post-critical set whose projection to is dense in the middle-third Cantor set.
2
Construction
Take a system of contraction similarities of , defined by
[TABLE]
and let be the attractor of . Here is infinite base-3 fraction beginning with 0.11 and containing all finite tuples, consisting of 0 and 2:
We will show that if is sufficiently small, then all the images , , are disjoint.
Put and denote by the set of all tuples formed by . Consider the images of under the maps . Using base-3 fractions, we can write them as , so for and for .
\Delta$$B$$A_{{{\bf j}}}$$h^{2}$$ch$$c$$c_{{{\bf j}}}$$c^{\prime}_{{{\bf j}}}$$\Delta_{{{\bf j}}}$$(0,0)$$(1,0)$$\ (c,h)$$\Delta^{\prime}_{{{\bf j}}}Figure 1.
Let be a triangle with vertices and . Since is not rational, the point is not equal to for any . So either or .
For , if lies in . To avoid this, the slope of the line has to be steeper than that of (See Fig 1.):
[TABLE]
similarly, for , we have to require that does not lie in
[TABLE]
So we need to estimate and .
Case 1. If , there are the following possibilities:
(a) = . Then -th entry . Since , then . So , , then .
(b) = for some and . Since the only entries allowed here are 0 and 2, so and . So and , therefore
Case 2. , then
(a) . Since , implies , so , , then .
(b) for some and . Then , , so , , so .
(c) if and i.e. , then .
Therefore
(d) if and , i.e. , we similarly get . Thus,
So if the inequalities (1) and (2) are satisfied. Further we show that if , the system satisfies open set condition(OSC) and one point intersection property and the attractor is a dendrite.
3 Proof of the Theorem.
Lemma 2**.**
If , for any , .
Proof. Let , . If for some and , then . It follows from and that and are disjoint. Thus .
If and for , then . By the construction, if , .
1/3$$2/3$$D$$\Delta$$D_{0}$$D_{1}$$D_{2}Fig. 2.
Lemma 3**.**
The system satisfies one point intersection property and open set condition(OSC).
Proof. Let be the interiors of and . Define . Obviously, for , . Moreover, .
Observe that with the only exception , the sets , and are disjoint. Since , the same is true for the sets and . But , so too, therefore are disjoint and (OSC) is fulfilled.
It follows from Lemma 2 that and therefore , which implies one point intersection property.
Lemma 4**.**
The system is post critically infinite and its post critical set is dense in the middle-third Cantor set .
Proof. Let be base 3 representation for some point from the middle-third Cantor set . Since the representation of contains all possible tuples of symbols 0 and 2, then for any there is such that for . Therefore . So, the sequence , converges to the point .
To finish the proof of the Theorem 1, we need only to check that the set is a dendrite. Let . This set is compact and it is simply-connected, because the sets are disjoint. It is a strong deformation retract of the set . Define . The sets form a nested sequence of compact simply-connected sets, each being a strong deformation retract of the previous one. Then the intersection is a strong deformation retract of the set . By Kigami’s theorem [4] it is locally connected and arcwise connected. Since the interior of is empty, it contains no simple closed curve, therefore it is a dendrite [2, Theorem 1.1].
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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- 2[2] Charatonik J., Charatonik W., Dendrites, Aportaciones Mat. Comun. 22 (1998), 227–253.
- 3[3] Hutchinson, J.E. Fractals and self-similarity . Indiana Univ. Math. J 30, 1981, 713-747
- 4[4] Kigami, J. Analysis on Fractals . Cambridge University Press, 2001
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