McMullen's 1998 paper 'Complex earthquakes and Teichmüller theory' (J. Amer. Math. Soc. 11, 283-320) posed four questions. Two are settled by later literature: the higher-dimensional grafting-bijection question was resolved by Scannell and Wolf, who proved that grafting by any fixed measured lamination is a homeomorphism of the Teichmüller space of every finite-type surface (harmonic-map method), with bending-lamination coordinates on Bers slices as a homeomorphism onto their image, complemented by Dumas and Wolf in the fixed-surface direction; and the conjectured rigidity of geometrically finite cone-manifolds with cone angles exceeding 2π2\pi was refuted by Izmestiev's compact infinitesimally flexible examples with all cone angles larger than 2π2\pi together with his non-isometric compact pairs having the same topology and equal cone angles. The two remaining open questions concern the interaction of the complex earthquake machinery with the PSL2(C)PSL_2(\mathbb{C}) character variety V(S)V(S): (1) does the bending holonomy ηλn(X)\eta_{\lambda_n}(X) of a fixed Riemann surface escape every compact subset of V(S)V(S) whenever the real parts of the complex measured laminations λn\lambda_n diverge, a statement known only when all λn\lambda_n are complex multiples of one fixed lamination; and (2) is the quasi-Fuchsian space QF(S)QF(S), known to be disk-convex, actually convex with respect to holomorphic functions on V(S)V(S)?

Background

Let SS be a closed, connected, orientable surface of genus g≥2g \geq 2. The Teichmüller space T(S)T(S) is the space of marked conformal structures on SS, equivalently marked complete hyperbolic structures; it is a complex manifold of dimension 3g−33g-3. The PSL2(C)PSL_2(\mathbb{C}) character variety V(S)V(S) parametrizes conjugacy classes of irreducible representations of the fundamental group π1(S)\pi_1(S) into PSL2(C)PSL_2(\mathbb{C}); in the source's convention V(S)V(S) is a complex manifold, of dimension 2dim⁡T(S)2 \dim T(S) (a complete hyperbolic 3-manifold M=H3/ρ(π1(S))M = \mathbb{H}^3/\rho(\pi_1(S)) is encoded by its holonomy representation ρ\rho). The quasi-Fuchsian space QF(S)⊂V(S)QF(S) \subset V(S) is the open subset of discrete faithful representations whose limit set is a quasicircle, that is, the image of a round circle under a quasiconformal homeomorphism of the Riemann sphere; by Bers simultaneous uniformization (as recorded in the source paper) QF(S)≅T(S)×T(Sˉ)QF(S) \cong T(S) \times T(\bar{S}), where Sˉ\bar{S} denotes SS with reversed orientation. A Bers slice is the subset of QF(S)QF(S) obtained by fixing one factor; transported by the Bers embedding — the classical holomorphic embedding of the Teichmüller space of the oppositely oriented surface into the finite-dimensional complex vector space Q(X)Q(X) of holomorphic quadratic differentials on a fixed X∈T(S)X \in T(S) — it becomes a bounded domain in Q(X)Q(X).

A measured geodesic lamination λ\lambda on a hyperbolic surface is a geodesic lamination (a closed union of disjoint simple geodesics) equipped with a transverse measure; the space ML(S)ML(S) of measured laminations is a piecewise-linear manifold in which weighted multicurves are dense. Thurston's earthquake twλ:T(S)→T(S)tw_\lambda: T(S) \to T(S) along λ\lambda is a leftward shearing deformation; grafting along λ\lambda inserts flat or projective bands along the leaves, producing another conformal structure. A complex projective structure on a surface is a geometric structure modelled on the projective geometry of CP1\mathbb{CP}^1 — concretely, an atlas of charts into CP1\mathbb{CP}^1 whose transition maps are restrictions of Möbius transformations in PSL2(C)PSL_2(\mathbb{C}) — and grafting together with bending data enters Thurston's parametrization of complex projective structures (see the exposition in Dumas's survey and in Scannell-Wolf). A complex measured lamination is a point of the quotient MLC(S)=(ML(S)×C)/ ⁣∼ML_{\mathbb{C}}(S) = (ML(S) \times \mathbb{C})/\!\sim, where (λ,z)∼(tλ,z/t)(\lambda, z) \sim (t\lambda, z/t) for t>0t > 0; its real part prescribes an earthquake and its imaginary part a bending, both supported on the same underlying lamination. For X∈T(S)X \in T(S), McMullen defined the bending holonomy η:MLC(S)×T(S)→V(S)\eta: ML_{\mathbb{C}}(S) \times T(S) \to V(S), ηλ(X)=ηi Im⁡λ(twRe⁡λ(X))\eta_\lambda(X) = \eta_{i\,\operatorname{Im}\lambda}(tw_{\operatorname{Re}\lambda}(X)) (formula (2.4) of the source), that is, the holonomy of the complex projective structure obtained from XX by performing the earthquake along the real part Re⁡λ\operatorname{Re}\lambda and then bending along the imaginary part Im⁡λ\operatorname{Im}\lambda. The path t↦ηtλ(X)t \mapsto \eta_{t\lambda}(X) for a fixed lamination λ\lambda is a complex earthquake; the source proves that earthquake paths extend to properly embedded earthquake disks in Teichmüller space (Theorem 1.1) and that ηtλ(X)\eta_{t\lambda}(X) escapes every compact subset of V(S)V(S) as ∣Re⁡t∣→∞|\operatorname{Re}t| \to \infty (Theorem 4.1 and Corollary 4.2), while for integral laminations the map is periodic in the imaginary direction, so no imaginary-direction divergence can hold.

For the convexity thread, recall that a subset KK of a complex space XX is disk-convex if every continuous map f:Δ‾→Xf: \overline{\Delta} \to X, holomorphic on the open unit disk Δ\Delta, with f(S1)⊂Kf(S^1) \subset K, satisfies f(Δ)⊂Kf(\Delta) \subset K. A stronger property, convexity with respect to holomorphic functions on XX, requires that for every compact C⊂KC \subset K the holomorphic hull {x∈X:∣f(x)∣≤sup⁡C∣f∣ for every function f holomorphic on X}\{x \in X : |f(x)| \leq \sup_C |f| \text{ for every function } f \text{ holomorphic on } X\} is contained in KK; the maximum principle applied to ff composed with a holomorphic disk shows that this property implies disk-convexity. Bers and Ehrenpreis proved that T(S)T(S) is holomorphically convex, meaning that the hull of every compact subset of T(S)T(S) with respect to the functions holomorphic on T(S)T(S) is again compact; and H. Shiga proved, in the 1984 paper that the source cites for this result, by an application of Grunsky's inequality for univalent (injective holomorphic) functions, that the Bers-embedded T(S)T(S) is convex with respect to holomorphic functions on the ambient vector space Q(X)Q(X). The source establishes that QF(S)QF(S) is disk-convex in V(S)V(S) (Theorem 5.1, called Theorem 1.2 in its introduction) and asks whether the stronger holomorphic-function convexity holds in the character-variety ambient.

For the settled threads of the bundle, two further notions are needed. First, a hyperbolic cone-manifold is a 3-manifold that is hyperbolic away from a singular locus LL consisting of disjoint closed geodesics along which the total dihedral angle (the cone angle) may differ from 2π2\pi; it is geometrically finite if it admits a finite-sided fundamental polyhedron, and every closed cone-manifold is geometrically finite with empty conformal boundary. Grafting produces cone-manifolds M(X,λ)M(X, \lambda) with cone angles 2(π+αi)>2π2(\pi + \alpha_i) > 2\pi when λ\lambda is supported on curves with weights αi\alpha_i, and McMullen's Conjecture 8.1 asserted that a geometrically finite cone-manifold is determined, up to isometry, by the topology of the pair, the parabolic locus (the cusp data, i.e. the conjugacy classes of parabolic subgroups of the fundamental group), the cone angles, and the conformal structure on the boundary. Second, for one-dimensional Teichmüller spaces the source proved that the complex earthquake map is a biholomorphism onto a sublevel set described by hyperbolic length (Theorem 1.3), that the grafting map grλ:T(S)→T(S)gr_\lambda: T(S) \to T(S) is a homeomorphism (Theorem 1.4), and that bending lamination plus a length ratio give coordinates on a punctured Bers slice (Theorem 1.5); its introduction asks whether Theorems 1.4 and 1.5 extend when dim⁡T(S)>1\operatorname{dim}T(S) > 1.

Problem Statement

Both questions below are posed for a closed, connected, orientable surface SS of genus g≥2g \geq 2 and take place in the PSL2(C)PSL_2(\mathbb{C}) character variety V(S)V(S) of π1(S)\pi_1(S). They are the two remaining open questions from McMullen's 1998 paper 'Complex earthquakes and Teichmüller theory' (Journal of the American Mathematical Society 11, 283-320); the source's other two questions (the extension of grafting bijectivity and bending coordinates beyond one-dimensional Teichmüller spaces, and the rigidity of geometrically finite cone-manifolds with cone angles exceeding 2π2\pi) are settled by later literature (Scannell and Wolf; Dumas and Wolf; Izmestiev). The source states its questions under the standing hypothesis that SS is a compact oriented surface of negative Euler characteristic (with boundary subgroups mapped to parabolics); the questions below concern the closed-surface case, with no boundary or parabolic data.

Question 1 (divergence of complex-earthquake holonomy; the Question at the end of section 4 of the source). Let X∈T(S)X \in T(S) be fixed. Recall MLC(S)=(ML(S)×C)/ ⁣∼ML_{\mathbb{C}}(S) = (ML(S) \times \mathbb{C})/\!\sim with (λ,z)∼(tλ,z/t)(\lambda, z) \sim (t\lambda, z/t) for t>0t > 0, that Re⁡λ\operatorname{Re}\lambda and Im⁡λ\operatorname{Im}\lambda denote the real and imaginary measured laminations of a complex measured lamination, and that ηλ(X)=ηi Im⁡λ(twRe⁡λ(X))\eta_\lambda(X) = \eta_{i\,\operatorname{Im}\lambda}(tw_{\operatorname{Re}\lambda}(X)) is the bending holonomy, obtained by earthquaking XX along Re⁡λ\operatorname{Re}\lambda and then bending along Im⁡λ\operatorname{Im}\lambda. Suppose λn∈MLC(S)\lambda_n \in ML_{\mathbb{C}}(S) is a sequence whose real parts diverge in ML(S)ML(S), that is, Re⁡λn\operatorname{Re}\lambda_n eventually leaves every compact subset of ML(S)ML(S). Is it true that ηλn(X)→∞\eta_{\lambda_n}(X) \to \infty in V(S)V(S), meaning that the sequence of holonomies eventually leaves every compact subset of the character variety? The known special case is a fixed lamination: ηtλ(X)→∞\eta_{t\lambda}(X) \to \infty in V(S)V(S) as ∣Re⁡t∣→∞|\operatorname{Re}t| \to \infty for every nonzero λ∈ML(S)\lambda \in ML(S) (source, Theorem 4.1 and Corollary 4.2); the general statement allows the underlying lamination and the imaginary part to vary arbitrarily with nn.

Question 2 (holomorphic-function convexity of quasi-Fuchsian space; the Question at the end of section 5 of the source). Is QF(S)QF(S) convex with respect to holomorphic functions on V(S)V(S)? Precisely: is it the case that for every compact subset C⊂QF(S)C \subset QF(S), the holomorphic hull C^={[ρ]∈V(S):∣f([ρ])∣≤sup⁡C∣f∣ for every function f holomorphic on V(S)}\widehat{C} = \{[\rho] \in V(S) : |f([\rho])| \leq \sup_C |f| \text{ for every function } f \text{ holomorphic on } V(S) \} is contained in QF(S)QF(S)? The source proves that QF(S)QF(S) is disk-convex in V(S)V(S) (Theorem 5.1); the present question asks for the strictly stronger hull-convexity property, in analogy with the classical theorem, recorded in the source's section 5 remarks, that the Bers-embedded T(S)T(S) is convex with respect to holomorphic functions on the ambient vector space of holomorphic quadratic differentials.

An answer, affirmative or negative, at this level of generality (in Question 1: arbitrary complex measured laminations with divergent real parts, arbitrary imaginary parts, any fixed X∈T(S)X \in T(S); in Question 2: arbitrary compact subsets of QF(S)QF(S); in both: any genus g≥2g \geq 2) resolves the corresponding question as stated, that is, the closed-surface instance of the source's question. The two questions are independent of one another.

References

  1. C. T. McMullen. Complex earthquakes and Teichmüller theory. Journal of the American Mathematical Society 11 (1998), no. 2, 283-320. DOI: 10.1090/s0894-0347-98-00259-8. URL: https://doi.org/10.1090/s0894-0347-98-00259-8. Full text also available at the author's site, https://people.math.harvard.edu/~ctm/papers/home/text/papers/graft/graft.pdf
  2. K. P. Scannell and M. Wolf. The grafting map of Teichmüller space. Journal of the American Mathematical Society 15 (2002), no. 4, 893-927. DOI: 10.1090/s0894-0347-02-00395-8. URL: https://doi.org/10.1090/s0894-0347-02-00395-8. Preprint arXiv:math/9810082, https://arxiv.org/abs/math/9810082
  3. D. Dumas and M. Wolf. Projective structures, grafting and measured laminations. Geometry & Topology 12 (2008), no. 1, 351-386. DOI: 10.2140/gt.2008.12.351. URL: https://doi.org/10.2140/gt.2008.12.351. Preprint arXiv:0712.0968, https://arxiv.org/abs/0712.0968
  4. D. Dumas. Complex Projective Structures (survey). Preprint arXiv:0902.1951, 2009. URL: https://arxiv.org/abs/0902.1951
  5. D. Dumas. Holonomy limits of complex projective structures. Advances in Mathematics 315 (2017), 427-473. DOI: 10.1016/j.aim.2017.05.021. URL: https://doi.org/10.1016/j.aim.2017.05.021. Preprint arXiv:1105.5102, https://arxiv.org/abs/1105.5102
  6. D. Dumas and R. P. Kent IV. Bers slices are Zariski dense. Journal of Topology 2 (2009), no. 2, 373-379. DOI: 10.1112/jtopol/jtp014. URL: https://doi.org/10.1112/jtopol/jtp014
  7. L. Bers and L. Ehrenpreis. Holomorphic convexity of Teichmüller spaces. Bulletin of the American Mathematical Society 70 (1964), no. 6, 761-764. DOI: 10.1090/s0002-9904-1964-11230-1. URL: https://doi.org/10.1090/s0002-9904-1964-11230-1
  8. H. Shiga. On analytic and geometric properties of Teichmüller spaces. Journal of Mathematics of Kyoto University 24 (1984), no. 3, 441-452. DOI: 10.1215/kjm/1250521274. URL: https://doi.org/10.1215/kjm/1250521274. (This is the paper cited as [Sh] in the source for the Grunsky-inequality convexity theorem of the Bers-embedded Teichmüller space.)
  9. H. Shiga. On analytic properties of deformation spaces of Kleinian groups. Transactions of the American Mathematical Society 368 (2016), no. 9, 6627-6642. DOI: 10.1090/tran/6563. URL: https://doi.org/10.1090/tran/6563.
  10. S. Gupta. On the asymptotic behavior of complex earthquakes and Teichmüller disks. In: Geometry, Groups and Dynamics, Contemporary Mathematics 639, American Mathematical Society, 2015, 271-287. DOI: 10.1090/conm/639/12820. URL: https://doi.org/10.1090/conm/639/12820. Preprint arXiv:1311.4933, https://arxiv.org/abs/1311.4933
  11. D. B. A. Epstein, A. Marden and V. Markovic. Complex earthquakes and deformations of the unit disk. Journal of Differential Geometry 73 (2006), no. 1, 119-166. DOI: 10.4310/jdg/1146680514. URL: https://doi.org/10.4310/jdg/1146680514
  12. C. T. McMullen. Navigating moduli space with complex twists. Journal of the European Mathematical Society 15 (2013), no. 4, 1223-1243. DOI: 10.4171/JEMS/390. URL: https://doi.org/10.4171/JEMS/390
  13. C. T. McMullen. Differential and algebraic geometry of earthquakes. Preprint dated 27 July 2026, available at the author's site, https://people.math.harvard.edu/~ctm/papers/home/text/papers/eq/eq.pdf
  14. C. D. Hodgson and S. P. Kerckhoff. Rigidity of hyperbolic cone-manifolds and hyperbolic Dehn surgery. Journal of Differential Geometry 48 (1998), no. 1, 1-59. DOI: 10.4310/jdg/1214460606. URL: https://doi.org/10.4310/jdg/1214460606
  15. S. Kojima. Deformations of hyperbolic 3-cone-manifolds. Journal of Differential Geometry 49 (1998), no. 3, 469-516. DOI: 10.4310/jdg/1214461108. URL: https://doi.org/10.4310/jdg/1214461108
  16. H. Weiss. Local rigidity of 3-dimensional cone-manifolds. Journal of Differential Geometry 71 (2005), no. 3, 437-506. DOI: 10.4310/jdg/1143571990. URL: https://doi.org/10.4310/jdg/1143571990
  17. H. Weiss. Global rigidity of 3-dimensional cone-manifolds. Journal of Differential Geometry 76 (2007), no. 3, 495-523. DOI: 10.4310/jdg/1180135696. URL: https://doi.org/10.4310/jdg/1180135696. Preprint arXiv:math/0504117, https://arxiv.org/abs/math/0504117
  18. K. Bromberg. Rigidity of geometrically finite hyperbolic cone-manifolds. Geometriae Dedicata 105 (2004), no. 1, 143-170. DOI: 10.1023/b:geom.0000024664.84428.e7. URL: https://doi.org/10.1023/b:geom.0000024664.84428.e7. Preprint arXiv:math/0009149, https://arxiv.org/abs/math/0009149
  19. R. Mazzeo and G. Montcouquiol. Infinitesimal rigidity of cone-manifolds and the Stoker problem for hyperbolic and Euclidean polyhedra. Journal of Differential Geometry 87 (2011), no. 3, 525-576. DOI: 10.4310/jdg/1312998235. URL: https://doi.org/10.4310/jdg/1312998235. Preprint arXiv:0908.2981, https://arxiv.org/abs/0908.2981
  20. I. Izmestiev. Examples of infinitesimally flexible 3-dimensional hyperbolic cone-manifolds. Journal of the Mathematical Society of Japan 63 (2011), no. 2, 581-598. DOI: 10.2969/jmsj/06320581. URL: https://doi.org/10.2969/jmsj/06320581. Preprint arXiv:0910.2876, https://arxiv.org/abs/0910.2876
  21. M. Bridgeman and K. Bromberg. Variation of holonomy for projective structures and an application to drilling hyperbolic 3-manifolds. Geometriae Dedicata 218 (2024), no. 3, article 62. DOI: 10.1007/s10711-024-00908-0. URL: https://doi.org/10.1007/s10711-024-00908-0. Preprint arXiv:2310.10890, https://arxiv.org/abs/2310.10890
  22. A. Casson. An example of weak non-rigidity for cone manifolds with vertices. Talk at the Third MSJ Regional Workshop, Tokyo, 1998 (unpublished; documented in the bibliography of Izmestiev's paper, https://arxiv.org/abs/0910.2876)
  23. S. Baba. Bending Teichmüller spaces and character varieties. Preprint arXiv:2203.15394, 2022. URL: https://arxiv.org/abs/2203.15394
  24. T. Cremaschi and V. Giovannini. Behaviour of the Schwarzian derivative on long complex projective tubes. Preprint arXiv:2502.10071, 2025. URL: https://arxiv.org/abs/2502.10071