2021
DOI: 10.1007/s00208-021-02148-z
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A Thurston boundary for infinite-dimensional Teichmüller spaces

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Cited by 6 publications
(7 citation statements)
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“…When X is a compact surface the space of geodesic currents G(X) is equipped with the standard weak* topology for which the Liouville map is an embedding onto its image (see Bonahon [3]). Bonahon and the second author [4] introduced the uniform weak* topology on the space of geodesic currents in order to introduce a Thurston boundary to Teichmüller spaces of arbitrary Riemann surfaces. This is a simplification of the topology that was introduced by the second author [10].…”
Section: The Liouville Map and Uniform Hölder Topologymentioning
confidence: 99%
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“…When X is a compact surface the space of geodesic currents G(X) is equipped with the standard weak* topology for which the Liouville map is an embedding onto its image (see Bonahon [3]). Bonahon and the second author [4] introduced the uniform weak* topology on the space of geodesic currents in order to introduce a Thurston boundary to Teichmüller spaces of arbitrary Riemann surfaces. This is a simplification of the topology that was introduced by the second author [10].…”
Section: The Liouville Map and Uniform Hölder Topologymentioning
confidence: 99%
“…The second author [10], and more recently, Bonahon and the second author [4] introduced the Thurston boundary to Teichmüller spaces of arbitrary conformally hyperbolic Riemann surfaces. In the case of an infinite area conformally hyperbolic Riemann surface, we need a uniform bound on deformations which was automatic for closed Riemann surfaces.…”
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confidence: 99%
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“…Geodesic currents also play a key step in the proof of rigidity of the marked length spectrum for metrics, via an argument by Otal [47, Théorème 2]. Finally, they provide a boundary of the Teichmüller space, in both the compact [8, Proposition 17] and noncompact [11, Theorem 2] cases.…”
Section: Introductionmentioning
confidence: 99%