Gromov-Witten invariants and Algebraic Geometry (II) Jun Li

Transcription

1 Gromov-Witten invariants and Algebraic Geometry (II) Shanghai Center for Mathematical Sciences and Stanford University

2 GW invariants of quintic Calabi-Yau threefolds Quintic Calabi-Yau threefolds: X = {w 5 = x x5 5 = 0} P 4 For d, g Z, form the moduli of stable maps M g (X, d) = {[f, C] f : C X, such that...}

3 Form virtual cycle [M g (X, d)] virt A 0 M g (X, d) The GW invariant N g (d) = 1 Q. [M g (X,d)] virt

4 The generating function f g (q) = N g (d)q d Determining it is a challenge to mathematicians

5 High genus invariants of quintics Recent progress toward an effective algorithm for all genus invariants using Mixed-Spin-P (MSP) fields. A joint work with Huailiang Chang, Weiping Li, and Mellisa Liu.

6 This work is inspired by Witten s vision that GW invariants of quintics and Witten s spin class invariants are equivalent via a wall crossing.

7 Witten s vision C acts on C 5 C of weight (1, 1, 1, 1, 1, 5); (x x 5 5 ) p : C5 C C is C equivariant; the quotient C 5 C/C is pretty bad;

8 Witten s vision C acts on C 5 C of weight (1, 1, 1, 1, 1, 5); (x x 5 5 ) p : C5 C C is C equivariant; the quotient C 5 C/C is pretty bad;

9 Witten s vision C acts on C 5 C of weight (1, 1, 1, 1, 1, 5); (x x 5 5 ) p : C5 C C is C equivariant; the quotient C 5 C/C is pretty bad;

10 Witten s vision [C 6 /C ] has two GIT quotients: (C 5 0) C/C = K P 4; C 5 (C 0)/C = C 5 /Z 5 ; we call (C 5 0) C/C and C 5 (C 0)/C related by a simple wall crossing.

11 Witten s vision [C 6 /C ] has two GIT quotients: (C 5 0) C/C = K P 4; C 5 (C 0)/C = C 5 /Z 5 ; we call (C 5 0) C/C and C 5 (C 0)/C related by a simple wall crossing.

12 Witten s vision [C 6 /C ] has two GIT quotients: (C 5 0) C/C = K P 4; C 5 (C 0)/C = C 5 /Z 5 ; we call (C 5 0) C/C and C 5 (C 0)/C related by a simple wall crossing.

13 Witten s vision Witten: a field theory valued in K P 4 is the GW of quintics; a field theory valued in C 5 /Z 5 is the Witten s spin class (FJRW invariants); these two theories are equivalent via a wall crossing. developed a (MSP) field theory realizing this wall crossing, an algorithm, conjecturally determine all genus invariants.

14 One side of this wall crossing: LG theory of K P 4 (with HL Chang) We constructed the GW invariants of stable maps with p-fields: M g (P 4, d) p = {[f, C, ρ] [f, C] M g (P 4, d), ρ H 0 (C, f O(5) ω C )} form its virtual cycle [M g (P 4, d) p ] virt loc define N g (d) p = [M g (P 4,d) p ] 1 Q virt loc

15 One side of this wall crossing: LG theory of K P 4 (with HL Chang) We constructed the GW invariants of stable maps with p-fields: M g (P 4, d) p = {[f, C, ρ] [f, C] M g (P 4, d), ρ H 0 (C, f O(5) ω C )} form its virtual cycle [M g (P 4, d) p ] virt loc define N g (d) p = [M g (P 4,d) p ] 1 Q virt loc

16 One side of this wall crossing: LG theory of K P 4 (with HL Chang) We constructed the GW invariants of stable maps with p-fields: M g (P 4, d) p = {[f, C, ρ] [f, C] M g (P 4, d), ρ H 0 (C, f O(5) ω C )} form its virtual cycle [M g (P 4, d) p ] virt loc define N g (d) p = [M g (P 4,d) p ] 1 Q virt loc

17 LG theory of K P 4 Theorem (Chang - L) The two sets of invariants are equivalent N g (d) = ( 1) d+g+1 N g (d) p. Up shot: N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves:

18 LG theory of K P 4 Theorem (Chang - L) The two sets of invariants are equivalent N g (d) = ( 1) d+g+1 N g (d) p. Up shot: N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves:

19 LG theory of K P 4 Theorem (Chang - L) The two sets of invariants are equivalent N g (d) = ( 1) d+g+1 N g (d) p. Up shot: N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves:

20 LG theory of K P 4 N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves: 1 definition says: counting of ([f : C P 4 ], ρ H 0 (C, f O(5) ω C )); 2 [f : C P 4 ] is (C, L, ϕ 1,, ϕ 5 ), where ϕ i H 0 (L) s.t. (ϕ 1,, ϕ 5 ) never zero; 3 the P-field ρ H 0 (L 5 ω C );

21 LG theory of K P 4 N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves: 1 definition says: counting of ([f : C P 4 ], ρ H 0 (C, f O(5) ω C )); 2 [f : C P 4 ] is (C, L, ϕ 1,, ϕ 5 ), where ϕ i H 0 (L) s.t. (ϕ 1,, ϕ 5 ) never zero; 3 the P-field ρ H 0 (L 5 ω C );

22 LG theory of K P 4 N g (d) are virtual counting of maps to the quintic X ; counting [f : C X P 4 ] N g (d) p is a virtual counting of fields on curves: 1 definition says: counting of ([f : C P 4 ], ρ H 0 (C, f O(5) ω C )); 2 [f : C P 4 ] is (C, L, ϕ 1,, ϕ 5 ), where ϕ i H 0 (L) s.t. (ϕ 1,, ϕ 5 ) never zero; 3 the P-field ρ H 0 (L 5 ω C );

23 LG theory of K P 4 N g (d) p is a virtual counting of fields because it v. counts (C, L, ϕ 1,, ϕ 5, ρ); they are fields taking values in K P 4 = (C 5 0) C/C because ϕ 1 H 0 (L) and ρ H 0 (L 5 ω C ), (compare) C acts on C 5 and C of weights 1 and 5; (ϕ 1,, ϕ 5 ) never zero and ρ arbitrary, (compare) (C 5 0) C/C ; the line bundle L is up to scaling, (compare) quotient by C. N g (d) p is a field theory taking values in K P 4 = (C 5 0) C/C.

24 LG theory of K P 4 N g (d) p is a virtual counting of fields because it v. counts (C, L, ϕ 1,, ϕ 5, ρ); they are fields taking values in K P 4 = (C 5 0) C/C because ϕ 1 H 0 (L) and ρ H 0 (L 5 ω C ), (compare) C acts on C 5 and C of weights 1 and 5; (ϕ 1,, ϕ 5 ) never zero and ρ arbitrary, (compare) (C 5 0) C/C ; the line bundle L is up to scaling, (compare) quotient by C. N g (d) p is a field theory taking values in K P 4 = (C 5 0) C/C.

25 LG theory of K P 4 N g (d) p is a virtual counting of fields because it v. counts (C, L, ϕ 1,, ϕ 5, ρ); they are fields taking values in K P 4 = (C 5 0) C/C because ϕ 1 H 0 (L) and ρ H 0 (L 5 ω C ), (compare) C acts on C 5 and C of weights 1 and 5; (ϕ 1,, ϕ 5 ) never zero and ρ arbitrary, (compare) (C 5 0) C/C ; the line bundle L is up to scaling, (compare) quotient by C. N g (d) p is a field theory taking values in K P 4 = (C 5 0) C/C.

26 The other side wall crossing: LG theory of C 5 /Z 5 It originated by Witten s class; The full theory has been developed by Fan-Jarvis-Ruan, called the FJRW invariants. (with HL Chang and WP Li) We provided a new construction of FJRW invariants (in narrow case).

27 The other side wall crossing: LG theory of C 5 /Z 5 It originated by Witten s class; The full theory has been developed by Fan-Jarvis-Ruan, called the FJRW invariants. (with HL Chang and WP Li) We provided a new construction of FJRW invariants (in narrow case).

28 LG theory of C 5 /Z 5 M g,γ (w 5, Z 5 ) p = { ( (Σ C, C), L, ϕ 1,, ϕ 5, ρ ) such that...} ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω C (Σ C )) ϕ i arbitrary, ρ nowhere vanishing. (compare) C 5 /Z 5 = C 5 (C 0)/C.

29 LG theory of C 5 /Z 5 M g,γ (w 5, Z 5 ) p = { ( (Σ C, C), L, ϕ 1,, ϕ 5, ρ ) such that...} ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω C (Σ C )) ϕ i arbitrary, ρ nowhere vanishing. (compare) C 5 /Z 5 = C 5 (C 0)/C.

30 LG theory of C 5 /Z 5 M g,γ (w 5, Z 5 ) p = { ( (Σ C, C), L, ϕ 1,, ϕ 5, ρ ) such that...} ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω C (Σ C )) ϕ i arbitrary, ρ nowhere vanishing. (compare) C 5 /Z 5 = C 5 (C 0)/C.

31 LG theory of C 5 /Z 5 Theorem (Chang - Li - L) The FJRW invariants can be constructed using cosection localized virtual cycles of the moduli of spin fields: M g,γ (w 5, Z 5 ) 5p = { ( Σ C, C, L, ϕ 1,, ϕ 5, ρ )... }/

32 Cosection technique The construction of the two theories 1 the GW invariants of stable maps with p-fields 2 the FJRW invariants of (w 5, Z 5 ) both rely on the construction of cosection localized virtual cyels; Theorem (Kiem - L) A DM stack M with a perfect obstruction theory, and a cosection σ : Ob M O M provides us a cosection localized virtual cycle (letting D(σ) = {σ = 0}) [M] virt σ A D(σ)

33 Cosection technique The construction of the two theories 1 the GW invariants of stable maps with p-fields 2 the FJRW invariants of (w 5, Z 5 ) both rely on the construction of cosection localized virtual cyels; Theorem (Kiem - L) A DM stack M with a perfect obstruction theory, and a cosection σ : Ob M O M provides us a cosection localized virtual cycle (letting D(σ) = {σ = 0}) [M] virt σ A D(σ)

34 Cosection technique Remark 1 The cosection localized virtual cycles allows one to construct invariants of non-compact moduli spaces; 2 The cosections used in the GW with p-fields and FJRW are induced by the same equivariant LG function (x x 5 5 ) p : C 5 C C.

35 Cosection technique Remark 1 The cosection localized virtual cycles allows one to construct invariants of non-compact moduli spaces; 2 The cosections used in the GW with p-fields and FJRW are induced by the same equivariant LG function (x x 5 5 ) p : C 5 C C.

36 Cosection technique The fields: ξ = (C, L, ϕ 1,, ϕ 5, ρ) H 0 (L) 5 H 0 (L 5 ω C ) The rel-obstruction space at ξ: ( ϕ, ρ) Ob ξ = H 1 (L) 5 H 1 (L 5 ω C ) The cosection σ ξ : Ob ξ C: Compare with σ ξ ( ϕ, ρ) = ρ x 5 i + ρ 5ϕ 4 i ϕ i H 1 (ω C ) = C. δ ( p (x x 5 5 ) ) = ρ x 5 i + ρ 5x 4 i ẋ i

37 Mixed Spin-P fields Next step is to geometrically realizing the wall crossing of these two field theories envisioned by Witten We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 )

38 Mixed Spin-P fields We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 ) where 1 (Σ C, C) is a pointed twisted curve, 2 L and N are line bundles, L as before, N is new; 3 ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω log ), as before; C 4 ν 1 H 0 (L N ), ν 2 H 0 (N ); 5 plus combined GIT like stability requirements.

39 Mixed Spin-P fields We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 ) where 1 (Σ C, C) is a pointed twisted curve, 2 L and N are line bundles, L as before, N is new; 3 ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω log ), as before; C 4 ν 1 H 0 (L N ), ν 2 H 0 (N ); 5 plus combined GIT like stability requirements.

40 Mixed Spin-P fields We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 ) where 1 (Σ C, C) is a pointed twisted curve, 2 L and N are line bundles, L as before, N is new; 3 ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω log ), as before; C 4 ν 1 H 0 (L N ), ν 2 H 0 (N ); 5 plus combined GIT like stability requirements.

41 Mixed Spin-P fields We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 ) where 1 (Σ C, C) is a pointed twisted curve, 2 L and N are line bundles, L as before, N is new; 3 ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω log ), as before; C 4 ν 1 H 0 (L N ), ν 2 H 0 (N ); 5 plus combined GIT like stability requirements.

42 Mixed Spin-P fields We define An MSP field = (Σ C, C, L, N, ϕ 1,, ϕ 5, ρ, ν 1, ν 2 ) where 1 (Σ C, C) is a pointed twisted curve, 2 L and N are line bundles, L as before, N is new; 3 ϕ i H 0 (C, L), ρ H 0 (C, L 5 ω log ), as before; C 4 ν 1 H 0 (L N ), ν 2 H 0 (N ); 5 plus combined GIT like stability requirements.

43 Moduli of MSP fields Theorem The moduli W g,γ,d of stable MSP-fields of 1 genus g = g(c); 2 monodromy γ = (γ 1,, γ l ) of L along Σ C, and 3 degrees d = (d 0, d ) (of L and N ) is a separated DM stack, locally of finite type.

44 Moduli of MSP fields Theorem The moduli W g,γ,d is a C stack, via (Σ C, C, L, N, ϕ, ρ, ν) t = (Σ C, C, L, N, ϕ, ρ, ν t ) where ν t = (tν 1, ν 2 ).

45 Moduli of MSP fields Theorem The moduli W g,γ,d has a C equivariant perfect obstruction theory, an equivariant cosection of its obstruction sheaf, thus an equivariant cosection localized virtual cycle [W g,γ,d ] virt loc AC W g,γ,d. where W g,γ,d = (σ = 0). A technical Lemma: (σ = 0) is compact.

46 Polynomial relations How to play with this cycle [W g,γ,d ] virt loc AC W g,γ,d Taking 1 γ = (no marked points), 2 (d 0, d ) = (d, 0), then [ Wg,d ] virt σ H C 2(d+1 g) (W g,d, Q).

47 Polynomial relations How to play with this cycle [W g,γ,d ] virt loc AC W g,γ,d Taking 1 γ = (no marked points), 2 (d 0, d ) = (d, 0), then [ Wg,d ] virt σ H C 2(d+1 g) (W g,d, Q).

48 Polynomial relations when d + 1 g > 0 [ Wg,d ] virt σ H C 2(d+1 g) (W g,d, Q). ( u d+1 g [W g,d ] virt σ ) 0 = 0.

49 Polynomial relations Let F Γ be the connected components of ( W g,d) C ; [u d+1 g [F Γ] virt ] σ Γ e(n FΓ ) = 0. 0 Γ for cosection localized version, proved by Chang-Kiem-L.

50 Polynomial relations [u d+1 g [F Γ] virt ] σ Γ e(n FΓ ) = 0. 0 Γ is a polynomial relation among (after proving a vanishing result), 1 GW invariants of the quintic Calabi-Yau N g (d); 2 FJRW invariants of (w 5, Z 5 ) with insertions 2 5 ; 3 Hodge integrals of M g,n involving ψ classes (calculable).

51 Polynomial relations Application I Letting d = 0, the relations provide an effective algorithm to evaluate the GW invariants N g (d) provided the following are known 1 FJRW invariants of insertions 2 5 and genus g g; 2 N g (d ) for (g, d ) such that g < g, and d d; 3 N g (d ) for d g.

52 Polynomial relations Application II Letting d 0 = 0, the relations provide an relations indexed by d > g 1 among FJRW invariants with insertions 2 5.

53 Forward looking Conjecture These relations, indexed by (d 0, d ) (with d 0 + d + 1 g > 0), provide an effective algorithm to determine all genus GW invariants and FJRW invariants of insertions 2 5.

54 Example III: GW technique to AG Conjecture: Any smooth projective complex K3 surface S contains infinitely many rational curves. This is motivated by Lang s conjecture: Lang Conjecture: Let X be a general type complex manifold. Then the union of the images of holomorphic u : C X lies in a finite union of proper subvarieties of X.

55 Example III: GW technique to AG Key to the existence of rational curves: A class α 0 H 2 (S, Z) is Hodge (i.e. H 1,1 (S, C) H 2 (S, Q)) is necessary and sufficient for the existence of a union of rational curves C i so that [C i ] = α. Example: Say we can have a family S t, t disk, α H 1,1 (S 0, C) H 2 (S 0, Q) so that S 0 has C 0 = CP 1 S 0 with [C 0 ] = α; in case α H 1,1 (S t, C) for general t, then CP 1 = C 0 S 0 can not be extended to holomorphic u t : CP 1 S t.

56 Example III: GW technique to AG We will consider polarized K3 surfaces (S, H), c 1 (H) > 0; we can group them according to H 2 = 2d: M 2d = {(S, H) H 2 = 2d}. each M 2d is smooth, of dimension 19; each M 2d is defined over Z. (defined by equation with coefficients in Z.) to show that (S, H) contains infinitely many rational curves, it suffices to show that for any N, there is a rational curve R S so that [R] H N. we define ρ(s) = dim H 1,1 (S, C) H 2 (S, Q), called the rank of the Picard group of S.

57 Extension Problem a family of polarized K3 surface (S t, H t ), t T (a parameter space); C 0 S 0 a union of rational curves; α = [C 0 ] = m[h t ] H 2 (S, Z); (a multiple of polarization); We like to show exists a family of curves C t S t, such that C t are union of rational curves; C 0 = C 0.

58 Extension Problem a family of polarized K3 surface (S t, H t ), t T (a parameter space); C 0 S 0 a union of rational curves; α = [C 0 ] = m[h t ] H 2 (S, Z); (a multiple of polarization); We like to show exists a family of curves C t S t, such that C t are union of rational curves; C 0 = C 0.

59 Extension Problem Use moduli of genus 0 stable maps represent C 0 S 0 as the image of [u 0 ] M 0 (S 0, α). Extension Lemma (Ran, Bogomolov-Tschinkel, ) Suppose [u 0 ] M 0 (S 0, α) is isolated, then u 0 extends to u t M 0 (S t, α) for general t T.

60 Extension Problem Definition: We say a map [u] M 0 (S, α) rigid if [u] is an isolated point in M 0 (S, α). Extension principle: In case (a genus zero stable map) u : C S is rigid, then u extends to nearby K3 surfaces as long as the class u [C] H 2 (S, Z) remains ample.

61 The existence theorem Theorem (Bogomolov - Hassett - Tschikel, L - Liedtke) Let (X, H) be a polarized complex K3 surface such that ρ(x ) is odd. Then X contains infinitely many rational curves.

62 The existence theorem Outline of proof We only need to prove the Theorem for (X, H) defined over a number field K; say K = Q, we get a family X p for every prime p Z, X is the generic member of this family; p, exists D p X p, D p ZH, we have sup D p H ; pick C p X p union of rationals, D p + C p n p H Difficulty: D p + C p may not be representable as the image of a rigid genus zero stable map.

63 The existence theorem Solution: Suppose we can find a nodal rational curves R X, of class kh for some k, then for some large m we can represent C p + D p + mr, which is a class in (n + mk)h, by a rigid genus zero stable map.

64 The existence theorem End of the proof: In general, X may not contain any nodal rational curve in kh. However, we know a small deformation of X in M 2d contains nodal rational curves in kh. Using this, plus some further algebraic geometry argument, we can complete the proof.

65 Thank you!