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In mathematics, '''Antoine's necklace''', discovered by {{harvs|txt=yes|authorlink= Louis Antoine|last=Antoine|first=Louis|year=1921}}, is an embedding of the [[Cantor set]] in 3-dimensional Euclidean space whose complement is not [[simply connected]].
{{Short description|Embedding of Cantor set in 3-dimensional Euclidean space}}
{{multiple image
| direction = vertical
| width = 200
| footer = Renderings of Antoine's necklace
| image1 = Antoine's Necklace Iteration 1.png
| alt1 = Antoine's necklace
| caption1 = First iteration
| image2 = Antoine's Necklace Iteration 2.png
| alt2 = Antoine's necklace
| caption2 = Second iteration
}}
In [[mathematics]], '''Antoine's necklace''' is a topological embedding of the [[Cantor set]] in 3-dimensional [[Euclidean space]], whose complement is not [[simply connected]]. It also serves as a counterexample to the claim that all [[Cantor space]]s are ambiently homeomorphic to each other. It was discovered by {{harvs|txt=yes|authorlink= Louis Antoine|last=Antoine|first=Louis|year=1921}}.<ref>{{citation|first=Louis|last=Antoine|authorlink=Louis Antoine|title=Sur l'homeomorphisme de deux figures et leurs voisinages
|journal= Journal de Mathématiques Pures et Appliquées|volume=4|year=1921|pages=221–325}}</ref>


==Construction==
It is constructed by starting with a [[solid torus]], replacing it by a "necklace" inside it formed of linked tori, then replacing each of these tori by another necklace inside it, and repeating this an infinite number of times.


Antoine's necklace is constructed iteratively like so: Begin with a [[solid torus]] ''A''<sup>0</sup> (iteration 0). Next, construct a "necklace" of smaller, linked tori that lie inside ''A''<sup>0</sup>. This necklace is ''A''<sup>1</sup> (iteration 1). Each torus composing ''A''<sup>1</sup> can be replaced with another smaller necklace as was done for ''A''<sup>0</sup>. Doing this yields ''A''<sup>2</sup> (iteration 2).
It was used by {{harvtxt|Alexander|1924}} to construct '''Antoine's horned sphere''' (similar to but not the same as [[Alexander's horned sphere]]).

==References==
This process can be repeated a countably infinite number of times to create an ''A''<sup>''n''</sup> for all ''n''. Antoine's necklace ''A'' is defined as the intersection of all the iterations.
*{{citation|first=Louis|last=Antoine|title=Sur l'homeomorphisme de deux figures et leurs voisinages

|journal= Journal Math Pures et appl.|volume=4|year=1921|pages=221–325}}
==Properties==
*{{citation|title=Remarks on a Point Set Constructed by Antoine

|authorlink=J. W. Alexander|first=J. W.|last= Alexander
Since the solid tori are chosen to become arbitrarily small as the iteration number increases, the connected components of ''A'' must be single points. It is then easy to verify that ''A'' is [[closure (mathematics)|closed]], [[dense-in-itself]], and [[totally disconnected]], having the [[cardinality of the continuum]]. This is sufficient to conclude that as an abstract metric space ''A'' is homeomorphic to the Cantor set.
|journal= Proceedings of the National Academy of Sciences of the United States of America

However, as a subset of Euclidean space ''A'' is not ambiently homeomorphic to the standard Cantor set ''C'', embedded in '''R'''<sup>3</sup> on a [[line segment]]. That is, there is no bi-continuous map from '''R'''<sup>3</sup> → '''R'''<sup>3</sup> that carries ''C'' onto ''A''. To show this, suppose there was such a map ''h'' : '''R'''<sup>3</sup> → '''R'''<sup>3</sup>, and consider a loop ''k'' that is interlocked with the necklace. ''k'' cannot be continuously shrunk to a point without touching ''A'' because two loops cannot be continuously unlinked. Now consider any loop ''j'' disjoint from ''C''. ''j'' can be shrunk to a point without touching ''C'' because we can simply move it through the gap intervals. However, the loop ''g'' = ''h''<sup>−1</sup>(''k'') is a loop that ''cannot'' be shrunk to a point without touching ''C'', which contradicts the previous statement. Therefore, ''h'' cannot exist.

In fact, there is no homeomorphism of '''R'''<sup>3</sup> sending ''A'' to a set of [[Hausdorff dimension]] < 1, since the complement of such a set must be simply-connected.

Antoine's necklace was used by {{harvs|txt|last=Alexander|first=James Waddell|authorlink=James Waddell Alexander II|year=1924}} to construct '''Antoine's horned sphere''' (similar to but not the same as [[Alexander's horned sphere]]).<ref>{{citation|title=Remarks on a Point Set Constructed by Antoine
|authorlink=James Waddell Alexander II|first=J. W.|last= Alexander
|journal= [[Proceedings of the National Academy of Sciences of the United States of America]]
|volume=10|issue= 1|year= 1924|pages= 10–12
|volume=10|issue= 1|year= 1924|pages= 10–12
|doi=10.1073/pnas.10.1.10|pmid=16576769|pmc=1085501|jstor=84203|bibcode=1924PNAS...10...10A|doi-access=free}}</ref> This construction can be used to show the existence of uncountably many embeddings of a disk or sphere into three-dimensional space, all inequivalent in terms of [[ambient isotopy]].<ref>{{citation|title=Antoine's Necklace or How to Keep a Necklace from Falling Apart
|doi=10.1073/pnas.10.1.10|pmid=16576769|pmc=1085501|jstor=84203}}
|first1= Beverly L. |last1=Brechner|first2= John C.|last2= Mayer
*{{citation|title=Antoine's Necklace or How to Keep a Necklace from Falling Apart
|first= Beverly L. |last=Brechner|first2= John C.|last2= Mayer
|journal= The College Mathematics Journal|volume= 19|issue= 4|year= 1988|pages= 306–320
|journal= The College Mathematics Journal|volume= 19|issue= 4|year= 1988|pages= 306–320
|doi=10.2307/2686463|jstor=2686463}}
|doi=10.2307/2686463|jstor=2686463}}</ref>

== See also ==

* {{annotated link|Cantor set#Cantor dust|Cantor dust}}
* {{annotated link|Knaster–Kuratowski fan}}
* {{annotated link|List of topologies}}
* {{annotated link|Sierpinski carpet}}
* {{annotated link|Whitehead manifold}}
* [[Wild knot]]
* [[Superhelix]]
* [[Hawaiian earring]]

==References==
{{reflist}}


==Further reading==
{{topology-stub}}
*{{cite book |last=Pugh |first=Charles Chapman |date=2002 |title=Real Mathematical Analysis |series=Undergraduate Texts in Mathematics |url=https://archive.org/details/realmathematical00char |url-access=registration |doi=10.1007/978-0-387-21684-3 |publisher=Springer New York |pages=[https://archive.org/details/realmathematical00char/page/106 106–108] |isbn=9781441929419}}


==External links==
[[Category: Topology]]
{{Sister project links|auto=y|wikt=}}


[[Category:Topology]]
[[fr:Collier d'Antoine]]
[[Category:Eponyms in geometry]]
[[Category:1921 introductions]]

Latest revision as of 06:58, 14 August 2024

Antoine's necklace
First iteration
Antoine's necklace
Second iteration
Renderings of Antoine's necklace

In mathematics, Antoine's necklace is a topological embedding of the Cantor set in 3-dimensional Euclidean space, whose complement is not simply connected. It also serves as a counterexample to the claim that all Cantor spaces are ambiently homeomorphic to each other. It was discovered by Louis Antoine (1921).[1]

Construction

[edit]

Antoine's necklace is constructed iteratively like so: Begin with a solid torus A0 (iteration 0). Next, construct a "necklace" of smaller, linked tori that lie inside A0. This necklace is A1 (iteration 1). Each torus composing A1 can be replaced with another smaller necklace as was done for A0. Doing this yields A2 (iteration 2).

This process can be repeated a countably infinite number of times to create an An for all n. Antoine's necklace A is defined as the intersection of all the iterations.

Properties

[edit]

Since the solid tori are chosen to become arbitrarily small as the iteration number increases, the connected components of A must be single points. It is then easy to verify that A is closed, dense-in-itself, and totally disconnected, having the cardinality of the continuum. This is sufficient to conclude that as an abstract metric space A is homeomorphic to the Cantor set.

However, as a subset of Euclidean space A is not ambiently homeomorphic to the standard Cantor set C, embedded in R3 on a line segment. That is, there is no bi-continuous map from R3R3 that carries C onto A. To show this, suppose there was such a map h : R3R3, and consider a loop k that is interlocked with the necklace. k cannot be continuously shrunk to a point without touching A because two loops cannot be continuously unlinked. Now consider any loop j disjoint from C. j can be shrunk to a point without touching C because we can simply move it through the gap intervals. However, the loop g = h−1(k) is a loop that cannot be shrunk to a point without touching C, which contradicts the previous statement. Therefore, h cannot exist.

In fact, there is no homeomorphism of R3 sending A to a set of Hausdorff dimension < 1, since the complement of such a set must be simply-connected.

Antoine's necklace was used by James Waddell Alexander (1924) to construct Antoine's horned sphere (similar to but not the same as Alexander's horned sphere).[2] This construction can be used to show the existence of uncountably many embeddings of a disk or sphere into three-dimensional space, all inequivalent in terms of ambient isotopy.[3]

See also

[edit]

References

[edit]
  1. ^ Antoine, Louis (1921), "Sur l'homeomorphisme de deux figures et leurs voisinages", Journal de Mathématiques Pures et Appliquées, 4: 221–325
  2. ^ Alexander, J. W. (1924), "Remarks on a Point Set Constructed by Antoine", Proceedings of the National Academy of Sciences of the United States of America, 10 (1): 10–12, Bibcode:1924PNAS...10...10A, doi:10.1073/pnas.10.1.10, JSTOR 84203, PMC 1085501, PMID 16576769
  3. ^ Brechner, Beverly L.; Mayer, John C. (1988), "Antoine's Necklace or How to Keep a Necklace from Falling Apart", The College Mathematics Journal, 19 (4): 306–320, doi:10.2307/2686463, JSTOR 2686463

Further reading

[edit]
[edit]