Abstract:We study projective structures on a surface having poles of prescribed orders. We obtain a monodromy map from a complex manifold parameterising such structures to the stack of framed PGL 2 (C) local systems on the associated marked bordered surface. We prove that the image of this map is contained in the union of the domains of the cluster charts. We discuss a number of open questions concerning this monodromy map.
“…In [4], we considered a moduli space parametrizing projective structures with poles of prescribed orders. To define such a projective structure, let us fix an ordinary projective structure P 0 on S. Then a meromorphic projective structure is defined as a collection of charts w : U → CP 1 given by ratios of solutions of the equation (2) as above, where now the quadratic differential φ is allowed to have poles.…”
Section: The Monodromy Map and Main Theoremmentioning
confidence: 99%
“…of degree 2 N where N is the number of marked points in the interior of S. In terms of the space Proj * (S, M), the main result of [4] was the following.…”
Section: The Monodromy Map and Main Theoremmentioning
confidence: 99%
“…First, we restrict attention to the open subset Proj • (S, M) ⊆ Proj(S, M), whose complement is the codimension 2 locus of projective structures with apparent singularities. We do this because the monodromy map of [4] is not defined at projective structures with apparent singularities. Second, we consider a finite cover…”
Section: Moduli Space Of Marked Projective Structuresmentioning
confidence: 99%
“…Then, for each puncture p, we can define a loop δ p ∈ π 1 (S, x) which travels from x to U (p) along β p , travels along a small loop around p in the counterclockwise direction, and then returns to x along β p . Lemma 6.2 [4,Lemma 4.2]. There is a bijection between the set of isomorphism classes of rigidified framed P GL 2 (C)-local systems on (S, M) and the set of points of the complex projective variety…”
Section: Moduli Space Of Framed Local Systemsmentioning
confidence: 99%
“…The framing at p is given by an eigenline of the monodromy, and hence for a generic framed local system, there is a unique way of modifying the framing at p to get a different framed local system. Lemma 6.5 [4,Lemma 9.4]. There is a birational action of the group (Z/2Z) P on the stack X (S, M) of framed local systems in which the nontrivial generator corresponding to p ∈ P acts by fixing the underlying local system and exchanging the two generically possible choices of framing at p.…”
We show that the Borel sums of the Voros symbols considered in the theory of exact WKB analysis arise naturally as Fock–Goncharov coordinates of framed PGL2false(double-struckCfalse)‐local systems on a marked bordered surface. Using this result, we show that these Borel sums can be extended to meromorphic functions on C∗, and we prove an asymptotic property of the monodromy map introduced in collaboration with Tom Bridgeland.
“…In [4], we considered a moduli space parametrizing projective structures with poles of prescribed orders. To define such a projective structure, let us fix an ordinary projective structure P 0 on S. Then a meromorphic projective structure is defined as a collection of charts w : U → CP 1 given by ratios of solutions of the equation (2) as above, where now the quadratic differential φ is allowed to have poles.…”
Section: The Monodromy Map and Main Theoremmentioning
confidence: 99%
“…of degree 2 N where N is the number of marked points in the interior of S. In terms of the space Proj * (S, M), the main result of [4] was the following.…”
Section: The Monodromy Map and Main Theoremmentioning
confidence: 99%
“…First, we restrict attention to the open subset Proj • (S, M) ⊆ Proj(S, M), whose complement is the codimension 2 locus of projective structures with apparent singularities. We do this because the monodromy map of [4] is not defined at projective structures with apparent singularities. Second, we consider a finite cover…”
Section: Moduli Space Of Marked Projective Structuresmentioning
confidence: 99%
“…Then, for each puncture p, we can define a loop δ p ∈ π 1 (S, x) which travels from x to U (p) along β p , travels along a small loop around p in the counterclockwise direction, and then returns to x along β p . Lemma 6.2 [4,Lemma 4.2]. There is a bijection between the set of isomorphism classes of rigidified framed P GL 2 (C)-local systems on (S, M) and the set of points of the complex projective variety…”
Section: Moduli Space Of Framed Local Systemsmentioning
confidence: 99%
“…The framing at p is given by an eigenline of the monodromy, and hence for a generic framed local system, there is a unique way of modifying the framing at p to get a different framed local system. Lemma 6.5 [4,Lemma 9.4]. There is a birational action of the group (Z/2Z) P on the stack X (S, M) of framed local systems in which the nontrivial generator corresponding to p ∈ P acts by fixing the underlying local system and exchanging the two generically possible choices of framing at p.…”
We show that the Borel sums of the Voros symbols considered in the theory of exact WKB analysis arise naturally as Fock–Goncharov coordinates of framed PGL2false(double-struckCfalse)‐local systems on a marked bordered surface. Using this result, we show that these Borel sums can be extended to meromorphic functions on C∗, and we prove an asymptotic property of the monodromy map introduced in collaboration with Tom Bridgeland.
We study a second-order linear differential equation known as the deformed cubic oscillator, whose isomonodromic deformations are controlled by the first Painlevé equation. We use the generalised monodromy map for this equation to give solutions to the Riemann-Hilbert problems of (Bridgeland in Invent Math 216(1):69–124, 2019) arising from the Donaldson-Thomas theory of the A$$_2$$
2
quiver. These are the first known solutions to such problems beyond the uncoupled case. The appendix by Davide Masoero contains a WKB analysis of the asymptotics of the monodromy map.
We consider a 3-Calabi–Yau triangulated category associated to an ideal triangulation of a marked bordered surface. Using the theory of harmonic maps between Riemann surfaces, we construct a natural map from a component of the space of Bridgeland stability conditions on this category to the enhanced Teichmüller space of the surface. We describe a relationship between the central charges of objects in the category and shear coordinates on the Teichmüller space.
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