FourierMukai partners and stability conditions on K3
surfaces
Heinrich Hartmann
University of Bonn
24.2.2011
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 1 / 19
Outline
1 Moduli spaces of sheaves on K3 surfaces
2 Stability conditions and the Kähler moduli space
3 Geometric interpretations of Ma's result
4 Future research plans
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 2 / 19
Moduli spaces on K3 surfaces are well behaved
Let X be a K3 surface and let N(X) = K(Coh(X))/rad(χ) be the
numerical K-group, endowed with the pairing (_._) = −χ(_, _).
Theorem (Mukai)
Let v ∈ N(X) be a vector with v.v = 0 and v.N(X) = Z. Then there
exists an ample class h ∈ NS(X) such that:
1 The moduli space M = Mh(v) is again a K3 surface.
In particular M is ne, smooth, compact and two-dimensional.
2 The FourierMukai functor is an equivalence:
ΦU : Db(M)
∼
−→ Db(X).
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 3 / 19
Ma interpretation of FourierMukai partners
Let X be a K3 surface. Recently, Shouhei Ma gave a surprising
interpretation of the set of FourierMukai partners of X:
Theorem (Ma)
There is a canonical bijection between
K3 surfaces Y
with Db(Y ) ∼= Db(X)
←→
standard cusps of the
Kähler moduli space KM(X)
.
There is a version for non-standard cusps and K3 surfaces twisted by
a Brauer class.
The proof uses deep theorems due to Mukai and Orlov to reduce the
statement to lattice theory.
Is there a geometric reason for this correspondence?
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 4 / 19
Construction of the Kähler moduli space
Consider the period domain
D(X) = { [z] ∈ P(N(X)C) | z.z = 0, z.¯z  0 } .
We and dene the Kähler moduli space to be
KM(X) = D(X)+
/Γ,
where Γ is the image of Aut(Db(X)) in O(N(X)).
The BailyBorel compactication KM(X) ⊂ KM(X) is a normal
projective variety. The complement KM(X)  KM(X) consists of
components of dimension 0 and 1 which are in bijection to Bi/Γ, where
Bi = { I ⊂ N(X) | primitive, isotropic, rk(I) = i + 1 }
for i = 0, 1 respectively.
Boundary components of dimension 0 are called cusps.
We call a cusp [I] ∈ KM(X) standard if I.N(X) = Z.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 5 / 19
Picture of the Kähler moduli space
Figure: Kähler moduli space with cusps, associated K3 surfaces and two dierent
degenerating paths.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 6 / 19
Bridgeland stability conditions
Let D be a C-linear, triangulated category.
Denition (Bridgeland)
A stability condition σ on D consists of:
a heart of a bounded t-structure A ⊂ D and
a vector z ∈ N(D)C, called central charge.
satisfying the following properties:
1 For all E ∈ A, E = 0 the complex number (z.[E]) = r exp(iπφ)
satises r  0 and φ ∈ (0, 1].
2 Existence of Hader-Narasimhan ltrations.
3 Local niteness.
An object E ∈ A is called σ-stable if for all sub-objects F ⊂ E in A
φ(F)  φ(E).
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 7 / 19
Stability conditions on K3 surfaces
Let X be a K3 surface and D = Db(X).
Theorem (Bridgeland)
The set of stability conditions Stab(D) on D has the structure of a
complex manifold. The map σ = (A, z) → z induces a Galois-cover
π : Stab†
(X) −→ P+
0 (X) ⊂
open
N(X)C,
where Stab†(X) is the connected component of Stab(D), containing the
stability conditions σX(ω, β). Moreover
Deck(π) ∼= Aut†
0(D)
is the group of auto-equivalences respecting the component Stab†(X) and
acting trivially on H∗(X, Z).
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 8 / 19
Stability conditions and the Kähler moduli space.
We get the following diagram
Stab†(X)
Gl+
2 (R)

π // P+
0 (X)
Gl+
2 (R)

Stab†(X)/Gl
+
2 (R) //
Aut†(D)

D+
0 (X)
Γ

Aut†(D)  Stab†(X)/Gl
+
2 (R)
π // KM0(X),
where KM0(X) ⊂ KM(X) is a special open subset, and Aut†(D) ⊂ Aut(D)
is the subgroup of auto-equivalences which respect the distinguished
component.
Fact: π is an isomorphism.
This fact has been stated by Bridgeland and Ma before. However, it seems
to depend on the following results.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 9 / 19
Equivalences respecting the distinguished component
Theorem
The following equivalences respect the distinguished component.
For a ne, compact, two-dimensional moduli space of Gieseker-stable
sheaves Mh(v), the FourierMukai equivalence induced by the
universal family.
The spherical twists along Gieseker-stable spherical vector bundles.
The spherical twists along OC(k) for a (−2)-curve C ⊂ X and k ∈ Z.
This allows us to show the following strengthening of a result of
[HuybrechtsMacriStellari].
Corollary
The map Aut†(Db(X)) −→ Γ ⊂ O(N(X)) is surjective.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 10 / 19
Main question
There is a canonical map
¯π : Stab†
(X) −→ KM(X).
What is the relation between stability conditions σ with ¯π(σ) near
to a cusp and the associated K3 surface Y ?
1 How is the heart of σ related to the heart Coh(Y )?
2 Can we construct Y as a moduli space of σ-stable objects?
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 11 / 19
Cusps and hearts
We can always nd a degeneration σ(t) of stability conditions, such that
the hearts converge to Coh(Y ):
Theorem
Let [I] ∈ KM(X) be a standard cusp and Y the K3 surface associated to
[I] via Ma's theorem. Then there exists a path σ(t) ∈ Stab†(X), t 0 and
an equivalence Φ : Db(Y )
∼
−→ D such that
1 lim
t→∞
π(σ(t)) = [I] ∈ KM(X) and
2 lim
t→∞
A(σ(t)) = Φ(Coh(Y )) as subcategories of D.
There are many other hearts that can occur as limits!
How can we classify all of them?
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 12 / 19
Linear degenerations
We dene a class of pahts γ(t) ∈ KM(X) called linear degeneration to
a cusp [I].
The prototypical example of a linear degeneration is ¯π(σY (β, tω)),
where σY (β, ω) is an explicit stability condition associated to
β, ω ∈ NS(X)R with ω ample, dened by Bridgeland.
Proposition
Let [v] ∈ KM(X) be a standard cusp and γ(t) ∈ KM(X) be a linear
degeneration to [v], then γ(t) is a geodesic converging to [v].
Conjecture
Every geodesic converging to [v] is a linear degeneration.
True in the Picard-rank one case
True if one works with BorelSerre compactication, c.f. [Borel-Ji].
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 13 / 19
Classication of linear degenerations
Theorem
Let [I] be a standard cusp of KM(X). Let σ(t) ∈ Stab†(X) be a path in
the stability manifold such that ¯π(σ(t)) ∈ KM(X) is a linear degeneration
to [I]. Let Y be the K3 surface associated to [v] by Ma. Then there exist
1 a derived equivalence Φ : Db(Y )
∼
−→ D,
2 classes β ∈ NS(Y )R, ω ∈ Amp(Y ) and
3 a path g(t) ∈ Gl
+
2 (R)
such that
σ(t) = Φ∗(σ∗
Y (β, t ω) · g(t))
for all t 0.
Moreover, the hearts of σ(t) · g(t)−1 are independent of t for t 0 and
can be explicitly described as a tilt of Coh(Y ).
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 14 / 19
Moduli of complexes on K3 surfaces
Let D be the derived category of a K3 surface X. For a stability condition
in the sense of Bridgeland σ ∈ Stab(D) and v ∈ N(D) we consider the
following moduli-space of semi-stable objects
Mσ
(v) = { E ∈ D | E σ-semi-stable, [E] = v } /even shifts.
This space has the structure of an Artin-stack of nite type due to results
by Lieblich and Toda. We prove the following result.
Theorem
If v ∈ N(X) is a vector with v.v = 0, v.N(X) = Z and σ ∈ Stab†(X) is
v-general stability condition, then:
1 The moduli space Mσ(v) is represented by a K3 surface X.
2 The universal family U ∈ Db(M × X) induces a derived equivalence
ΦU : Db(M)
∼
−→ Db(X).
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 15 / 19
Immediate open questions:
Are all geodesics to cusps linear degenerations?
Borel and Ji show, that our linear degenerations are the
EDM-geodesics in the BorelSerre compactication of D(X)/Γ.
Study bers of the morphism
D(X)/Γ
BS
−→ D(X)/Γ
BB
= KM(X).
Is the stability manifold connected?
Do all auto-equivalences of Db(X) preserve the component Stab†(X)?
Open cases are:
Unstable spherical vector bundles
Moduli spaces of simple bundles
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 16 / 19
Cusps on abelian surfaces
Can Ma's theorem be generalized to other (CalabiYau)-varieties?
Abelian surfaces A are the rst test case.
The stability manifold has been described by Bridgeland:
Stab†
(A) −→ P+
(A)
is the universal cover.
The auto-equivalences of abelian varieties known by Orlov and
Polishchuk
0 −→ Z ⊕ (A × ˆA) −→ Aut(Db(A)) −→ U(A × ˆA) −→ 0,
where U(A × ˆA) ⊂ Aut(A × ˆA) is a certain explicit subgroup.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 17 / 19
Automorphic functions on the stability manifold
The Kähler moduli space
KM0(X) = Aut†
(X)  Stab†
(X)/Gl
+
2 (R)
is a quasi-projective variety. Sections of an ample line bundle give rise
to automorphic functions on the stability manifold.
Use DonaldsonThomas/Joyce invariants DTα(v) to construct
interesting functions on the stability manifold. (c.f. Toda,
MellitOkada)
Study Fourier-expansion of these functions at various cusps.
Already interesting in Picard-rank one case, where
KM(X) ∼= H/Γ+
0 (n)
is a Fricke modular curve.
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 18 / 19
Periods and Fano manifolds
In an other work we computed the mirror map
φ : KM(X)
∼
−→ CM(Y )
between the Kähler moduli space of a generic quartic X ⊂ P3 and the
complex deformation space of the mirror K3 surface (Dwork pencil).
We have KM(X) ∼= H/Γ+
0 (2) and CM(Y ) ∼= P1  {0, 1, ∞}, therefore
φ gives rise to a modular function ˜φ : H −→ C.
The function ˜φ is explicitly given as a quotient of solutions to the
PicardFuchs equation ˜φ = W1/W2.
By Mirror symmetry for the Fano manifold P3 the the PicardFuchs
equation for Y equals the Quantum dierential equation for P3.
The solutions W1, W2 can be constructed directly in terms of
GromovWitten invariants. (KatzarkovKontsevichPantev, Iritani)
Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 19 / 19

More Related Content

PDF
Pushforward of Differential Forms
PDF
Lattices of Lie groups acting on the complex projective space
PDF
Presentacion granada
PDF
Information geometry: Dualistic manifold structures and their uses
PDF
An elementary introduction to information geometry
PDF
Perspectives on the wild McKay correspondence
PDF
Matrix Models of 2D String Theory in Non-trivial Backgrounds
PDF
The wild McKay correspondence
Pushforward of Differential Forms
Lattices of Lie groups acting on the complex projective space
Presentacion granada
Information geometry: Dualistic manifold structures and their uses
An elementary introduction to information geometry
Perspectives on the wild McKay correspondence
Matrix Models of 2D String Theory in Non-trivial Backgrounds
The wild McKay correspondence

What's hot (19)

PDF
Postdoctoral research statement
PPT
Combinatorial Conditions For The Rigidity Of Tensegrity Frameworks By Recski
PDF
Lesson 27: Evaluating Definite Integrals
PDF
Computing F-blowups
PDF
PDF
Multiple integrals
PDF
Internal workshop jub talk jan 2013
PPT
Rigidity And Tensegrity By Connelly
PDF
E42012426
PDF
11. gamma sag semi ti spaces in topological spaces
PDF
Gamma sag semi ti spaces in topological spaces
PDF
presentation-geseke
PDF
8 fixed point theorem in complete fuzzy metric space 8 megha shrivastava
PDF
10.1.1.226.4381
PDF
Lesson 30: The Definite Integral
DOCX
Digital text
PDF
Homogeneous Components of a CDH Fuzzy Space
PDF
RW-CLOSED MAPS AND RW-OPEN MAPS IN TOPOLOGICAL SPACES
PDF
Some Fixed Point Theorems in b G -cone Metric Space
Postdoctoral research statement
Combinatorial Conditions For The Rigidity Of Tensegrity Frameworks By Recski
Lesson 27: Evaluating Definite Integrals
Computing F-blowups
Multiple integrals
Internal workshop jub talk jan 2013
Rigidity And Tensegrity By Connelly
E42012426
11. gamma sag semi ti spaces in topological spaces
Gamma sag semi ti spaces in topological spaces
presentation-geseke
8 fixed point theorem in complete fuzzy metric space 8 megha shrivastava
10.1.1.226.4381
Lesson 30: The Definite Integral
Digital text
Homogeneous Components of a CDH Fuzzy Space
RW-CLOSED MAPS AND RW-OPEN MAPS IN TOPOLOGICAL SPACES
Some Fixed Point Theorems in b G -cone Metric Space
Ad

Similar to Cusps of the Kähler moduli space and stability conditions on K3 surfaces (20)

PDF
slides_thesis
PDF
deformations of smooth functions on 2-torus whose kronrod-reeb graph is a tree
PDF
introtogaugetheory.pdf
PDF
Doubled Geometry and Double Field Theory
PDF
Slides: The dual Voronoi diagrams with respect to representational Bregman di...
PDF
Analytic construction of points on modular elliptic curves
PDF
Optimization introduction
PDF
Reflect tsukuba524
PDF
Analysis and algebra on differentiable manifolds
PDF
M. Visinescu: Hidden Symmetries of the Five-dimensional Sasaki - Einstein Spaces
PDF
Seminar on Motivic Hall Algebras
PDF
cswiercz-general-presentation
PDF
PDF
Dr NV SRINIVASULU-Tpjrc ijaerd paper
PDF
Notes on Intersection theory
PDF
Hk3114251433
PDF
On learning statistical mixtures maximizing the complete likelihood
PDF
Frobenious theorem
PPTX
8 beam deflection
PDF
Reciprocity Law For Flat Conformal Metrics With Conical Singularities
slides_thesis
deformations of smooth functions on 2-torus whose kronrod-reeb graph is a tree
introtogaugetheory.pdf
Doubled Geometry and Double Field Theory
Slides: The dual Voronoi diagrams with respect to representational Bregman di...
Analytic construction of points on modular elliptic curves
Optimization introduction
Reflect tsukuba524
Analysis and algebra on differentiable manifolds
M. Visinescu: Hidden Symmetries of the Five-dimensional Sasaki - Einstein Spaces
Seminar on Motivic Hall Algebras
cswiercz-general-presentation
Dr NV SRINIVASULU-Tpjrc ijaerd paper
Notes on Intersection theory
Hk3114251433
On learning statistical mixtures maximizing the complete likelihood
Frobenious theorem
8 beam deflection
Reciprocity Law For Flat Conformal Metrics With Conical Singularities
Ad

More from Heinrich Hartmann (19)

PDF
Latency SLOs Done Right @ SREcon EMEA 2019
PDF
Circonus: Design failures - A Case Study
PDF
Linux System Monitoring with eBPF
PDF
Statistics for Engineers
PDF
Scalable Online Analytics for Monitoring
PDF
Geometric Aspects of LSA
PDF
Geometric Aspects of LSA
PDF
Seminar on Complex Geometry
PDF
GROUPOIDS, LOCAL SYSTEMS AND DIFFERENTIAL EQUATIONS
PDF
Topics in Category Theory
PDF
Related-Work.net at WeST Oberseminar
PDF
Komplexe Zahlen
PDF
Dimensionstheorie Noetherscher Ringe
PDF
Polynomproblem
PDF
Hecke Curves and Moduli spcaes of Vector Bundles
PDF
Dimension und Multiplizität von D-Moduln
PDF
Nodale kurven und Hilbertschemata
PDF
Local morphisms are given by composition
PPTX
Latency SLOs Done Right @ SREcon EMEA 2019
Circonus: Design failures - A Case Study
Linux System Monitoring with eBPF
Statistics for Engineers
Scalable Online Analytics for Monitoring
Geometric Aspects of LSA
Geometric Aspects of LSA
Seminar on Complex Geometry
GROUPOIDS, LOCAL SYSTEMS AND DIFFERENTIAL EQUATIONS
Topics in Category Theory
Related-Work.net at WeST Oberseminar
Komplexe Zahlen
Dimensionstheorie Noetherscher Ringe
Polynomproblem
Hecke Curves and Moduli spcaes of Vector Bundles
Dimension und Multiplizität von D-Moduln
Nodale kurven und Hilbertschemata
Local morphisms are given by composition

Recently uploaded (20)

PPTX
Introduction to Immunology (Unit-1).pptx
PPT
Mutation in dna of bacteria and repairss
PPT
Cell Structure Description and Functions
PPTX
PMR- PPT.pptx for students and doctors tt
PPTX
Preformulation.pptx Preformulation studies-Including all parameter
PDF
Worlds Next Door: A Candidate Giant Planet Imaged in the Habitable Zone of ↵ ...
PDF
Cosmology using numerical relativity - what hapenned before big bang?
PDF
CuO Nps photocatalysts 15156456551564161
PPTX
Presentation1 INTRODUCTION TO ENZYMES.pptx
PPTX
Introcution to Microbes Burton's Biology for the Health
PPT
LEC Synthetic Biology and its application.ppt
PDF
Unit 5 Preparations, Reactions, Properties and Isomersim of Organic Compounds...
PDF
Communicating Health Policies to Diverse Populations (www.kiu.ac.ug)
PPTX
ELISA(Enzyme linked immunosorbent assay)
PPTX
LIPID & AMINO ACID METABOLISM UNIT-III, B PHARM II SEMESTER
PPTX
SCIENCE 4 Q2W5 PPT.pptx Lesson About Plnts and animals and their habitat
PPTX
Cells and Organs of the Immune System (Unit-2) - Majesh Sir.pptx
PPT
THE CELL THEORY AND ITS FUNDAMENTALS AND USE
PDF
From Molecular Interactions to Solubility in Deep Eutectic Solvents: Explorin...
PPT
Enhancing Laboratory Quality Through ISO 15189 Compliance
Introduction to Immunology (Unit-1).pptx
Mutation in dna of bacteria and repairss
Cell Structure Description and Functions
PMR- PPT.pptx for students and doctors tt
Preformulation.pptx Preformulation studies-Including all parameter
Worlds Next Door: A Candidate Giant Planet Imaged in the Habitable Zone of ↵ ...
Cosmology using numerical relativity - what hapenned before big bang?
CuO Nps photocatalysts 15156456551564161
Presentation1 INTRODUCTION TO ENZYMES.pptx
Introcution to Microbes Burton's Biology for the Health
LEC Synthetic Biology and its application.ppt
Unit 5 Preparations, Reactions, Properties and Isomersim of Organic Compounds...
Communicating Health Policies to Diverse Populations (www.kiu.ac.ug)
ELISA(Enzyme linked immunosorbent assay)
LIPID & AMINO ACID METABOLISM UNIT-III, B PHARM II SEMESTER
SCIENCE 4 Q2W5 PPT.pptx Lesson About Plnts and animals and their habitat
Cells and Organs of the Immune System (Unit-2) - Majesh Sir.pptx
THE CELL THEORY AND ITS FUNDAMENTALS AND USE
From Molecular Interactions to Solubility in Deep Eutectic Solvents: Explorin...
Enhancing Laboratory Quality Through ISO 15189 Compliance

Cusps of the Kähler moduli space and stability conditions on K3 surfaces

  • 1. FourierMukai partners and stability conditions on K3 surfaces Heinrich Hartmann University of Bonn 24.2.2011 Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 1 / 19
  • 2. Outline 1 Moduli spaces of sheaves on K3 surfaces 2 Stability conditions and the Kähler moduli space 3 Geometric interpretations of Ma's result 4 Future research plans Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 2 / 19
  • 3. Moduli spaces on K3 surfaces are well behaved Let X be a K3 surface and let N(X) = K(Coh(X))/rad(χ) be the numerical K-group, endowed with the pairing (_._) = −χ(_, _). Theorem (Mukai) Let v ∈ N(X) be a vector with v.v = 0 and v.N(X) = Z. Then there exists an ample class h ∈ NS(X) such that: 1 The moduli space M = Mh(v) is again a K3 surface. In particular M is ne, smooth, compact and two-dimensional. 2 The FourierMukai functor is an equivalence: ΦU : Db(M) ∼ −→ Db(X). Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 3 / 19
  • 4. Ma interpretation of FourierMukai partners Let X be a K3 surface. Recently, Shouhei Ma gave a surprising interpretation of the set of FourierMukai partners of X: Theorem (Ma) There is a canonical bijection between K3 surfaces Y with Db(Y ) ∼= Db(X) ←→ standard cusps of the Kähler moduli space KM(X) . There is a version for non-standard cusps and K3 surfaces twisted by a Brauer class. The proof uses deep theorems due to Mukai and Orlov to reduce the statement to lattice theory. Is there a geometric reason for this correspondence? Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 4 / 19
  • 5. Construction of the Kähler moduli space Consider the period domain D(X) = { [z] ∈ P(N(X)C) | z.z = 0, z.¯z 0 } . We and dene the Kähler moduli space to be KM(X) = D(X)+ /Γ, where Γ is the image of Aut(Db(X)) in O(N(X)). The BailyBorel compactication KM(X) ⊂ KM(X) is a normal projective variety. The complement KM(X) KM(X) consists of components of dimension 0 and 1 which are in bijection to Bi/Γ, where Bi = { I ⊂ N(X) | primitive, isotropic, rk(I) = i + 1 } for i = 0, 1 respectively. Boundary components of dimension 0 are called cusps. We call a cusp [I] ∈ KM(X) standard if I.N(X) = Z. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 5 / 19
  • 6. Picture of the Kähler moduli space Figure: Kähler moduli space with cusps, associated K3 surfaces and two dierent degenerating paths. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 6 / 19
  • 7. Bridgeland stability conditions Let D be a C-linear, triangulated category. Denition (Bridgeland) A stability condition σ on D consists of: a heart of a bounded t-structure A ⊂ D and a vector z ∈ N(D)C, called central charge. satisfying the following properties: 1 For all E ∈ A, E = 0 the complex number (z.[E]) = r exp(iπφ) satises r 0 and φ ∈ (0, 1]. 2 Existence of Hader-Narasimhan ltrations. 3 Local niteness. An object E ∈ A is called σ-stable if for all sub-objects F ⊂ E in A φ(F) φ(E). Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 7 / 19
  • 8. Stability conditions on K3 surfaces Let X be a K3 surface and D = Db(X). Theorem (Bridgeland) The set of stability conditions Stab(D) on D has the structure of a complex manifold. The map σ = (A, z) → z induces a Galois-cover π : Stab† (X) −→ P+ 0 (X) ⊂ open N(X)C, where Stab†(X) is the connected component of Stab(D), containing the stability conditions σX(ω, β). Moreover Deck(π) ∼= Aut† 0(D) is the group of auto-equivalences respecting the component Stab†(X) and acting trivially on H∗(X, Z). Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 8 / 19
  • 9. Stability conditions and the Kähler moduli space. We get the following diagram Stab†(X) Gl+ 2 (R) π // P+ 0 (X) Gl+ 2 (R) Stab†(X)/Gl + 2 (R) // Aut†(D) D+ 0 (X) Γ Aut†(D) Stab†(X)/Gl + 2 (R) π // KM0(X), where KM0(X) ⊂ KM(X) is a special open subset, and Aut†(D) ⊂ Aut(D) is the subgroup of auto-equivalences which respect the distinguished component. Fact: π is an isomorphism. This fact has been stated by Bridgeland and Ma before. However, it seems to depend on the following results. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 9 / 19
  • 10. Equivalences respecting the distinguished component Theorem The following equivalences respect the distinguished component. For a ne, compact, two-dimensional moduli space of Gieseker-stable sheaves Mh(v), the FourierMukai equivalence induced by the universal family. The spherical twists along Gieseker-stable spherical vector bundles. The spherical twists along OC(k) for a (−2)-curve C ⊂ X and k ∈ Z. This allows us to show the following strengthening of a result of [HuybrechtsMacriStellari]. Corollary The map Aut†(Db(X)) −→ Γ ⊂ O(N(X)) is surjective. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 10 / 19
  • 11. Main question There is a canonical map ¯π : Stab† (X) −→ KM(X). What is the relation between stability conditions σ with ¯π(σ) near to a cusp and the associated K3 surface Y ? 1 How is the heart of σ related to the heart Coh(Y )? 2 Can we construct Y as a moduli space of σ-stable objects? Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 11 / 19
  • 12. Cusps and hearts We can always nd a degeneration σ(t) of stability conditions, such that the hearts converge to Coh(Y ): Theorem Let [I] ∈ KM(X) be a standard cusp and Y the K3 surface associated to [I] via Ma's theorem. Then there exists a path σ(t) ∈ Stab†(X), t 0 and an equivalence Φ : Db(Y ) ∼ −→ D such that 1 lim t→∞ π(σ(t)) = [I] ∈ KM(X) and 2 lim t→∞ A(σ(t)) = Φ(Coh(Y )) as subcategories of D. There are many other hearts that can occur as limits! How can we classify all of them? Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 12 / 19
  • 13. Linear degenerations We dene a class of pahts γ(t) ∈ KM(X) called linear degeneration to a cusp [I]. The prototypical example of a linear degeneration is ¯π(σY (β, tω)), where σY (β, ω) is an explicit stability condition associated to β, ω ∈ NS(X)R with ω ample, dened by Bridgeland. Proposition Let [v] ∈ KM(X) be a standard cusp and γ(t) ∈ KM(X) be a linear degeneration to [v], then γ(t) is a geodesic converging to [v]. Conjecture Every geodesic converging to [v] is a linear degeneration. True in the Picard-rank one case True if one works with BorelSerre compactication, c.f. [Borel-Ji]. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 13 / 19
  • 14. Classication of linear degenerations Theorem Let [I] be a standard cusp of KM(X). Let σ(t) ∈ Stab†(X) be a path in the stability manifold such that ¯π(σ(t)) ∈ KM(X) is a linear degeneration to [I]. Let Y be the K3 surface associated to [v] by Ma. Then there exist 1 a derived equivalence Φ : Db(Y ) ∼ −→ D, 2 classes β ∈ NS(Y )R, ω ∈ Amp(Y ) and 3 a path g(t) ∈ Gl + 2 (R) such that σ(t) = Φ∗(σ∗ Y (β, t ω) · g(t)) for all t 0. Moreover, the hearts of σ(t) · g(t)−1 are independent of t for t 0 and can be explicitly described as a tilt of Coh(Y ). Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 14 / 19
  • 15. Moduli of complexes on K3 surfaces Let D be the derived category of a K3 surface X. For a stability condition in the sense of Bridgeland σ ∈ Stab(D) and v ∈ N(D) we consider the following moduli-space of semi-stable objects Mσ (v) = { E ∈ D | E σ-semi-stable, [E] = v } /even shifts. This space has the structure of an Artin-stack of nite type due to results by Lieblich and Toda. We prove the following result. Theorem If v ∈ N(X) is a vector with v.v = 0, v.N(X) = Z and σ ∈ Stab†(X) is v-general stability condition, then: 1 The moduli space Mσ(v) is represented by a K3 surface X. 2 The universal family U ∈ Db(M × X) induces a derived equivalence ΦU : Db(M) ∼ −→ Db(X). Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 15 / 19
  • 16. Immediate open questions: Are all geodesics to cusps linear degenerations? Borel and Ji show, that our linear degenerations are the EDM-geodesics in the BorelSerre compactication of D(X)/Γ. Study bers of the morphism D(X)/Γ BS −→ D(X)/Γ BB = KM(X). Is the stability manifold connected? Do all auto-equivalences of Db(X) preserve the component Stab†(X)? Open cases are: Unstable spherical vector bundles Moduli spaces of simple bundles Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 16 / 19
  • 17. Cusps on abelian surfaces Can Ma's theorem be generalized to other (CalabiYau)-varieties? Abelian surfaces A are the rst test case. The stability manifold has been described by Bridgeland: Stab† (A) −→ P+ (A) is the universal cover. The auto-equivalences of abelian varieties known by Orlov and Polishchuk 0 −→ Z ⊕ (A × ˆA) −→ Aut(Db(A)) −→ U(A × ˆA) −→ 0, where U(A × ˆA) ⊂ Aut(A × ˆA) is a certain explicit subgroup. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 17 / 19
  • 18. Automorphic functions on the stability manifold The Kähler moduli space KM0(X) = Aut† (X) Stab† (X)/Gl + 2 (R) is a quasi-projective variety. Sections of an ample line bundle give rise to automorphic functions on the stability manifold. Use DonaldsonThomas/Joyce invariants DTα(v) to construct interesting functions on the stability manifold. (c.f. Toda, MellitOkada) Study Fourier-expansion of these functions at various cusps. Already interesting in Picard-rank one case, where KM(X) ∼= H/Γ+ 0 (n) is a Fricke modular curve. Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 18 / 19
  • 19. Periods and Fano manifolds In an other work we computed the mirror map φ : KM(X) ∼ −→ CM(Y ) between the Kähler moduli space of a generic quartic X ⊂ P3 and the complex deformation space of the mirror K3 surface (Dwork pencil). We have KM(X) ∼= H/Γ+ 0 (2) and CM(Y ) ∼= P1 {0, 1, ∞}, therefore φ gives rise to a modular function ˜φ : H −→ C. The function ˜φ is explicitly given as a quotient of solutions to the PicardFuchs equation ˜φ = W1/W2. By Mirror symmetry for the Fano manifold P3 the the PicardFuchs equation for Y equals the Quantum dierential equation for P3. The solutions W1, W2 can be constructed directly in terms of GromovWitten invariants. (KatzarkovKontsevichPantev, Iritani) Heinrich Hartmann (University of Bonn) FourierMukai partners and stability conditions on K3 surfaces24.2.2011 19 / 19