2020
DOI: 10.1017/etds.2020.43
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Big mapping class groups and rigidity of the simple circle

Abstract: Let $\unicode[STIX]{x1D6E4}$ denote the mapping class group of the plane minus a Cantor set. We show that every action of $\unicode[STIX]{x1D6E4}$ on the circle is either trivial or semiconjugate to a unique minimal action on the so-called simple circle.

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Cited by 15 publications
(20 citation statements)
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“…When S = R 2 , Lemmas 6.6 and 6.8 from [10] show that the normal closure of Γ (r) is equal to Γ. This proves N div = Γ = Γ 0 in the special case of S = R 2 since each mapping class in Γ (r) is supported in a dividing disk in this situation.…”
Section: An Immediate Corollary Ismentioning
confidence: 73%
See 1 more Smart Citation
“…When S = R 2 , Lemmas 6.6 and 6.8 from [10] show that the normal closure of Γ (r) is equal to Γ. This proves N div = Γ = Γ 0 in the special case of S = R 2 since each mapping class in Γ (r) is supported in a dividing disk in this situation.…”
Section: An Immediate Corollary Ismentioning
confidence: 73%
“…First note that N div ⊂ Γ 0 since each mapping class supported in a disk becomes trivial under the forgetful map to Mod(S). To prove the converse, we shall use notation and terminology consistent with [10]. Recall that a short ray in S is an isotopy class of proper embedded ray from ∞ to some point in K, and a lasso is a homotopically essential properly embedded copy of R in S from ∞ to ∞.…”
Section: An Immediate Corollary Ismentioning
confidence: 99%
“…In this topology, the property of a ray having a (transverse) self-intersection is open. Thus the set of simple rays is closed on S 1 C , and is also nowhere dense [6,Lemma 3.3].…”
Section: Background On Rays and Loopsmentioning
confidence: 99%
“…Relationship to the ray graph. The ray graph was introduced by Calegari in [5] and is defined as follows. The ray graph is the graph whose vertex set is the set of isotopy classes of proper rays, with interior in the complement of the Cantor set K ⊂ R 2 , from a point in K to infinity, and whose edges (of length 1) are the pairs of such rays that can be realized disjointly.…”
Section: Introductionmentioning
confidence: 99%