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International Mathematics Research Notices, Vol. 2009, No. 24, pp. 4597–4625 Advance Access publication June 27, 2009

doi:10.1093/imrn/rnp101

Moduli of Bundles over Rational Surfaces and Elliptic Curves II: Nonsimply Laced Cases

Naichung Conan Leung

1

and Jiajin Zhang

2

1

Institute of Mathematical Sciences and Department of Mathematics, The Chinese University of Hong Kong, Hong Kong and

2

Department of Mathematics, Sichuan University, Chengdu, 610000, People’s Republic of China

Correspondence to be sent to: [email protected]

For any nonsimply laced Lie groupGand elliptic curve, we show that the moduli space of flat G bundles over can be identified with the moduli space of rational surfaces with G-configurations which contain as an anticanonical curve. We also construct Lie(G)-bundles over these surfaces. The corresponding results for simply laced groups were obtained by the authors in another paper. Thus, we have established a natural identification for these two kinds of moduli spaces for any Lie groupG.

1 Introduction

There is a classical identification for the moduli space of flat En bundles over a fixed elliptic curveand the moduli space of del Pezzo surfaces of degree 9−ncontainingas an anticanonical curve (see [3–6]). For other simply laced Lie groupG, that is, Lie group of ADE type, we also obtained in [13] an identification for the moduli space of flatGbundles over a fixed elliptic curveand the moduli space of the pairs (S,), whereSis a rational surface (calledADE-surface in [13]) containingas an anticanonical curve. In this paper, we extend the above identification to nonsimply laced cases. Therefore, we establish

Received November 21, 2008; Accepted June 8, 2009 Communicated by Prof. Dragos Oprea

C The Author 2009. Published by Oxford University Press. All rights reserved. For permissions, please e-mail: [email protected].

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a one-to-one correspondence between flatG bundles over a fixed elliptic curve and rational surfaces with as an anticanonical curve for Lie groups ofalltypes.

A nonsimply laced Lie groupGis uniquely determined by a simply laced Lie group Gand its outer automorphism group. Hence, it is natural to apply the previous results for the simply laced cases in [13] to the current situation. Similar to simply laced cases, we can defineG-surfacesandrational surfaces with G-configurations (see Definitions 3.3, 3.8, 3.13, 3.19). Our main result is the following.

Theorem 1.1. Letbe a fixed elliptic curve with identity 0∈,Gbe any simple, com- pact, simply connected and nonsimply laced Lie group. DenoteS(,G) the moduli space of the pairs (S,), where Sis aG-surface such that∈ | −KS|. DenoteMG the moduli space of flatG-bundles over. Then we have

(i) S(,G) can be embedded intoMGas an open dense subset.

(ii) This embedding can be extended to an isomorphism fromS(,G) ontoMG by including all rational surfaces withG-configurations, and this gives us a natural and explicit compactificationS(,G) ofS(,G).

This paper is motivated by some duality in physics. When G=En is a simple subgroup ofE8×E8, theseG bundles are related to the duality between F-theory and string theory. Among other things, this duality predicts that the moduli of flatEnbundles over a fixed elliptic curvecan be identified with the moduli of del Pezzo surfaces with fixed anticanonical curve . For details, one can consult [3, 4, 6]. Our result can be considered as a test of the above duality for other Lie groups.

As an application, this identification provides us with an intuitive explanation forMG. We also provide an interesting geometric realization of root system theory, and we can see very clearly how the Weyl group acts on the (marked) moduli space of flat G-bundles over.

In the following, we illustrate briefly via pictures whatG-configurations andG- surfaces are in each case and compare it with the corresponding case whereGis simply laced.

1.1 Bn-configurations as specialDn+1-configurations

In these cases we consider rational surfaces with fibration structure and a fixed smooth anticanonical curve . A Bn-configuration comes from a Dn+1-configuration. Roughly speaking, by saying a rational surfaceShas a Dn+1-configuration (l1,. . .,ln+1), we mean that S can be considered as a blowup of F1 (a Hirzebruch surface) at n+1 points on

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f l1

· · · ln+ 1

0

fl1 fl2

· · · x1

−x1 Σ

l2

x2

−x2

S P SO(2n+ 2)

1

Fig. 1. A surface with aDn+1-configuration (l1,. . .,ln+1).

f l1

l2

· · · ln+1

0 x1

x2

−x2

fl1 fl2

S

1

Σ SO(2n+ 1)

Fig. 2. A surface with aBn-configuration (l1,l2,. . .,ln+1), wherex1=l1=0.

∈ | −KF1|, such thatl1,. . .,ln+1 are the corresponding exceptional classes [13]. When these blown-up points arein general position,Sis called aG=Dn+1-surface. See Figure 1 for a surface with a Dn+1-configuration.

Given a surface S with a Dn+1-configuration ζ =(l1,. . .,ln+1), if it satisfies the condition x1=l1, which is the identity element zero of the elliptic curve, thenζ is a Bn-configuration on S(Definition 3.3). If all blown-up points but x1 are in general position,Sis called a Bn-surface. See Figure 2 for a surface with a Bn-configuration.

1.2 Cn-configurations as special A2n−1-configurations

In these cases, we consider rational surfaces with fibration and section structure and a fixed smooth anticanonical curve.

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s

f l1

· · · · · ·

ln ln+1 l2n

0 x1

−x1

Σ

S

P1 s SU(2n)

Fig. 3. A surface with anA2n−1-configuration (l1,. . .,l2n).

f

0

S

P1 s s

l1

· · · ln

l1 ln

−x1 −xn

x1 xn Σ

Sp(n)

Fig. 4. A surface with aCn-configuration (l1,. . .,ln,ln,. . .,l1).

ACn-configuration comes from anA2n1-configuration. By saying that a rational surfaceShas an A2n1-configuration (l1,. . .,l2n), we mean that Scan be considered as a blowup ofF1at 2npoints on ∈ | −KF1|which sum to zero, such thatl1,. . .,l2nare the corresponding exceptional classes [13]. When these blown-up points arein general posi- tion,Sis called anA2n−1-surface. See Figure 3 for a surface with anA2n−1-configuration.

Given a surface S with an A2n1-configuration ζ =(l1,. . .,l2n), if it satisfies the conditionxi = −x2n+1iwithxi =li, fori=1,. . .,n, thenζis called aCn-configuration on S (Definition 3.8). If all blown-up points are in general position, S is called a Cn- surface. See Figure 4 for a surface with aCn-configuration.

1.3 G2-configurations as specialD4-configurations

In these cases we still consider rational surfaces with fibration structure and a fixed smooth anticanonical curve.

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f l4

0

−x4

x4

l2 l3

l1

x1

−x1

Σ

S P1 SO(8)

Fig. 5. A surface with aD4-configuration (l1,. . .,l4).

f l1

l2 l3 l4

0 x1

x2 x3 x4

S

P1 Σ

G2

Fig. 6. A surface with aG2-configuration (l1,l2,l3,l4), wherex1=0 andx4=x2+x3withxi=li. A G2-configuration comes from a D4-configuration. We have seen what a D4- configuration is from Section 1.1 of the Introduction. Roughly speaking, by saying that a rational surfaceShas a D4-configuration (l1,. . .,l4), we mean thatScan be considered as a blowup ofF1at four points on∈ | −KF1|, such thatl1,. . .,l4are the corresponding exceptional classes [13]. When these blown-up points arein general position,Sis called aG=D4-surface. See Figure 5 for a surface with a D4-configuration.

Given a surface Swith a D4-configuration ζ =(l1,. . .,l4), if it satisfies two con- ditions x1=0 andx4=x2+x3, where xi =li, thenζ is called aG2-configuration on S (Definition 3.13). If all blown-up points but x1 are in general position, S is called a G2-surface. See Figure 6 for a surface with aG2-configuration.

1.4 F4-configurations as special E6-configurations

In these cases we consider rational surfaces which are blowups of the projective planeP2 at six points in almost general position and which contain a fixed smooth anticanonical curve [13].

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0

l1 l2 l3 l4 l5 l6

S

Σ E6

Fig. 7. A surface with anE6-configuration (l1,. . .,l6).

0 l1 l6

l2

l5

l3

l4

L16 L25

L34

p S

Σ F4

Fig. 8. A surface with anF4-configuration (l1,. . .,l6), where three linesL16,L25,L34meet atp, or equivalently,x1+x6=x2+x5=x3+x4withxi=li.

An F4-configuration comes from an E6-configuration. Recall that by saying a rational surfaceShas anE6-configuration (l1,. . .,l6), we mean that Scan be considered as a blowup ofP2at six points on∈ | −KP2|, such thatl1,. . .,l6are the corresponding exceptional classes. When these blown-up points are in general position, S is called an E6-surface, which is in fact a cubic surface. See Figure 7 for a surface with an E6- configuration.

Given a surfaceSwith anE6-configurationζ =(l1,. . .,l6), if it satisfies the condi- tionx1+x6=x2+x5=x3+x4, wherexi =li, thenζis called anF4-configuration onS (Definition 3.19). If all blown-up points arein general position,Sis called anF4-surface.

See Figure 8 for a surface with anF4-configuration.

Moreover, we can constructG=Lie(G) bundles overSwith aG-configuration. By restriction, we obtain Lie(G) bundles over . And we can also construct some natural fundamental representation bundles over, which have interesting geometric meanings, such that the Lie algebra bundles are the automorphism bundles of these representation bundles preserving certain algebraic structures.

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In this paper, the notations are the same as those in [13]. Let G be a compact, simple, and simply connected Lie group. We denote

r(G): the rank ofG;

R(G): the root system;

Rc(G): the coroot system;

W(G): the Weyl group;

(G): the root lattice;

c(G): the coroot lattice;

w(G): the weight lattice;

T(G): a maximal torus;

ad(G): the adjoint group ofG, i.e.G/C(G), whereC(G) is the center ofG;

(G): a simple root system ofG; and

Out(G): the outer automorphism group ofG, which is defined as the quotient of the automorphism group of G by its inner automorphism group. It is well known that Out(G) is isomorphic to the diagram automorphism group of the Dynkin diagram ofG.

When there is no confusion, we just ignore the letterG.

2 Reductions to Simply Laced Cases

LetGbe any simple, compact, and simply connected Lie group. ThenGis classified into the following seven types according to its Lie algebra:

(1) An-type,G=SU(n+1);

(2) Bn-type,G=Spin(2n+1);

(3) Cn-type,G=Sp(n);

(4) Dn-type,G=Spin(2n);

(5) En-type,n=6, 7, 8;

(6) F4-type; and (7) G2-type.

Among these,An,Dn, andEnare of simply laced type, whileBn,Cn,F4, andG2are of nonsimply laced type. And An,Bn,Cn,Dnare called classical Lie groups, whileEn,F4, andG2are called exceptional Lie groups.

From now on, we always assume thatGis a compact, simple, simply connected Lie group of nonsimply laced type, that is, of type Bn,Cn,F4,G2. There are two natural approaches to reduce situations to simply laced cases. One is embeddingGinto a simply laced Lie groupGsuch thatGis the subgroup fixed by the outer automorphism group ofG. Another is taking the simply laced subgroupGof maximal rank.

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In the following, we explain the first reduction. The following result is well known.

Proposition 2.1. Let G be a compact, nonsimply laced, simple, and simply connected Lie group. There exists a simple, simply connected, and simply laced Lie groupG, s.t.

GGandG=(G)ρ, whereρis an outer automorphism ofGof order three forG=D4, and of order two otherwise.

Proof. By the functorial property, we just need to prove it in the Lie algebra level. For the construction ofG=Lie(G) and G=Lie(G), one can see [10] for details, where the construction of Lie algebras is determined by the construction of root systems.

Remark. For later use, we list the construction of nonsimply laced root systems via simply laced root systems.

1. G=Cn=Sp(n),G=A2n1=SU(2n).

(G)= {αi,i=1,. . ., 2n−1}.

Out(G)= {1,ρ} ∼=Z2, whereρ(αi)=α2ni,i=1,. . .,n−1,ρ(αn)=αn. (G)= {βi = 12(αi+α2ni),i=1,. . .,n−1,βn=αn}.

2. G=Bn=Spin(2n+1),G=Dn+1=Spin(2n+2).

(G)= {αi,i=1,. . .,n+1}.

Out(G)= {1,ρ} ∼=Z2, whereρ(αi)=αi,i=3,. . .,n+1,ρ(α1)=α2,ρ(α2)=α1. (G)= {β1= 12(α1+α2),βi =αi+1,i=2,. . .,n}.

3. G=F4,G=E6.

(G)= {αi,i=1,. . ., 6}.

Out(G)= {1,ρ} ∼=Z2, whereρ(αi)=α6i,i=1,. . ., 5, andρ(α6)=α6. (G)= {β1= 12(α1+α5),β2=12(α2+α4),β3=α3,β4=α6}.

4. G=G2,G=D4=Spin(8).

(G)= {αi,i=1,. . ., 4}.

Out(G)= ρ1,ρ2 ∼=S3, whereρ1interchangesα1andα2, andρ2interchanges α1andα4.

(G)= {β1= 13(α1+α2+α4),β2=α3}. The Dynkin diagrams ofGandGare given in Figure 9.

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<

G G

Cn A2n−1

β1 β2 βn−1 βn α1 α2 αn α2n−2 α2n−1

>

Bn Dn+1

βn βn−1 β2 β1 αn+1 αn α3

α2

α1

<

F4 E6

β1 β2 β3 β4 α1 α2 α3 α4 α5

α6

<

G2 D4

β1 β2 α1 α2 α3

α4

Fig. 9. Nonsimply lacedGreduced to simply lacedG.

Remark. Note thatW(G) is the subgroup ofW(G) fixing the root systemR(G) and also the subgroup pointwise fixed by Out(G). For a root α, let SαW(G) be the reflection with respect to α, that is, Sα(x)=x+(x,α)α. Thus, as a subgroup of W(A2n1),W(Cn) is generated by SαiSα2n−i for i=1,. . .,n−1 and Sαn. As a subgroup of W(Dn+1),W(Bn) is generated by Sα1Sα2 and Sαi for i=3,. . .,n+1. As a subgroup of W(E6),W(F4) is generated bySα1Sα5,Sα2Sα4,Sα3andSα6. As a subgroup ofW(D4),W(G2) is generated by Sα1Sα2Sα4 andSα3.

In the following, let be a fixed elliptic curve with identity element 0, and fix a primitivedth root of Jac()∼=, whered =2 for Dncase,d =9−nfor Encase, and d=n+1 for An case, respectively (see [13]). Recall that for any compact, simple, and simply connected Lie group H, the moduli space of flat Hbundles overis

MH ∼=(c(H)⊗)/W(H).

ForG, the group Out(G) acts on

(c(G)⊗)/W(G) naturally. Let ((c(G)⊗)/W(G))Out(G)be the fixed part.

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Then, we have a natural map

χ : (c(G)⊗)/W(G)→((c(G)⊗)/W(G))Out(G). The image ofχis contained in a connected component of the fixed part.

Lemma 2.2. The map

χ : (c(G)⊗)/W(G)→((c(G)⊗)/W(G))Out(G) is injective.

Proof. It suffices to prove that for anyx,y(G)⊗, if∃wW(G), such thatw(x)=y, then∃wW(G), such thatw(x)=y. ForAnandDncases, this is obvious if we check the root lattices. For E6 case, we can also check it directly with the help of computer. Of course, we can also check this case by hand following the discussion in Section 2.4.1.

Corollary 2.3. (i) The fixed part ((c(G)⊗)/W(G))Out(G)is determined by the condi- tionρ(x)=x, up toW(G)-action, where xc(G)⊗, andρ is a generator ofOut(G), of order three forG=D4and of order two forG= An, En.

(ii) The moduli spaceMG∼=(c(G)⊗)/W(G) is a connected component of the fixed part

MGOut(G)∼=((c(G)⊗)/W(G))Out(G)

containing the trivialGbundle.

Proof. (i) For any xc(G)⊗, denote by ¯x the class in (c(G)⊗)/W(G). Then ρ( ¯x)=x¯ if and only if there exists wW(G), such that ρ(x)=w(x). Thus, w1ρ(x)=x.

Butw1ρOut(G) sinceOut(G)=Aut(G)/W(G). Thus, we can take a new simple root system such thatw1ρis the generator of the diagram automorphism (the automorphism of order three forD4).

(ii) By (i), (c(G)⊗)/W(G) and (MG)Out(G) are both orbifolds with the same dimension. Thus, the result follows from Lemma 2.2.

If we express the moduli space of flatGbundles overas (T×T)/W(G), where T is a maximal torus ofG, then we have the following corollary.

Corollary 2.4. If two elements ofT×T are conjugate under W(G), then they are also conjugate underW(G).

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Another method is to reduceGto its simply laced subgroupGof maximal rank, and apply the results for simply laced cases to current situation. In another occasion, we will discuss our moduli space ofG-bundles from this aspect in detail. Here, we just mention the following well-known fact from Lie theory.

Proposition 2.5. There exists canonically a simply laced Lie subgroupGofG, which is of maximal rank, that is,GandGshare a common maximal torus. And there is a short exact sequence

1→W(G)→W(G)Out(G)→1,

where Out(G) is the outer automorphism group of G. Thus, if we write the moduli space asMG=(T×T)/W, then

MG=MG/Out(G).

Remark. We give this construction ofGin each case.

(1) ForG=Sp(n), G=SU(2)n. Out(G) is the group Sn of permutations of the ncopies ofSU(2) inG.

(2) For G=G2, G=SU(3). Out(G) is the groupZ2that exchanges the three- dimensional representation of SU(3) with its dual.

(3) ForG=Spin(2n+1), G=Spin(2n).Out(G) is the groupZ2that exchanges the two spin representations ofSpin(2n).

(4) ForG=F4, G=Spin(8).Out(G) is the triality group S3that permutes the three eight-dimensional representations ofSpin(8).

3 FlatGBundles over Elliptic Curves and Rational Surfaces: Nonsimply Laced Cases In this section, we study case by case the G bundles over elliptic curves and rational surfaces for a nonsimply laced Lie groupG.

3.1 TheBn(n≥2) bundles

According to the arguments of the previous section, for G=Spin(2n+1) we can take G=Spin(2n+2), such thatG=(G)Out(G).

Let S=Yn+1be a rational surface with a Dn+1-configuration [13] which contains as a smooth anticanonical curve. Recall [13] thatYn+1is a blowup ofF1atn+1 points x1,. . .,xn+1 on, with corresponding exceptional classesl1,. . .,ln+1. Let f be the class

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of fibers inF1, and s be the section such that 0=s is the identity element of . The Picard group ofYn+1is H2(Yn+1,Z), which is a lattice with basiss, f,l1,. . .,ln+1. The canonical line bundleK= −(2s+3fn+1

i=1li).

We know from [13] that

Pn+1:= {xH2(Yn+1,Z)|x·K=x· f=0} is a root lattice ofDn+1type. We take a simple root system ofGas

(Dn+1)= {α1=l1l2,α2= fl1l2,α3=l2l3,. . .,αn+1=lnln+1}.

Letρ be the generator of Out(G)∼=Z2, such thatρ(α1)=α2,ρ(α2)=α1andρ(αi)=αi for i=3,. . .,n+1.

From [13], we know that the pair (S,) determines a homomorphism uH om((G),)

which is given by the restriction map

u(α)=O(α)|.

Lemma 3.1. LetuH om((G),) correspond to a pair (S,), whereSis a surface with aDn+1-configuration. Thenρ·u=uif and only if 2x1=0.

Proof. Since u is the restriction map: αiO(αi)|,u(α1)=O(l1l2)|=x1x2, and u(α2)=O(fl1l2)|= −x1x2. Hence, ρ·u=uu(α1)=u(α2)⇔x1x2= −x1x2⇔2x1=0⇔x1is one of the four points of order two on the elliptic curve.

As in [13], we denote byS(,G) the moduli space ofG=Dn+1-surfaces with a fixed anticanonical curve, and by S(,G) the natural compactification by including all rational surfaces with Dn+1-configurations (Figure 1). From [13], we know that φ: S(,G)−→ MG is an isomorphism.

Corollary 3.2. For uMG →(MG)Out(G), φ1(u)∈S(,G) represents a class of sur- facesYn+1(x1,. . .,xn+1) withx1=0, and such a surface corresponds to a boundary point in the moduli space, that is,φ1(u)∈S(,G)\S(,G).

Proof. By Lemma 3.1, u∈(MG)Out(G) if and only if 2x1=0. There are four con- nected components corresponding to four points of order two on . SinceMG is the component containing the trivial G bundle, we have x1=0. Recall (Section 4 of [13])

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thatYn+1(x1,. . .,xn+1)∈S(,G) if and only if 0,x1,. . .,xn+1are in general position, which implies in particularx1=0. Hence,φ−1(u) corresponds to a boundary point.

DenoteS=Yn+1(x1=0,x2,. . .,xn+1) (orYn+1for brevity) the blowup ofF1atn+1 pointsx1=0,x2,. . .,xn+1on, with exceptional divisorsl1,l2,. . .,ln+1, where∈ | −KS|.

Similar to the simply laced cases, we give the following definition.

Definition 3.3. ABn-exceptional systemonSis ann-tuple (e1,e2,. . .,en+1), whereei’s are exceptional divisors such thatei·ej =0=ei· f,i= jandy1=e1=0 is the identity of . A Bn-configuration on S is a Bn-exceptional system ζBn=(e1,e2,. . .,en+1) such that we can consider Sas a blowup of F1 atn+1 points y1=0,y2,. . .,yn+1 on , that is S=Yn+1(y1=0,y2,. . .,yn+1), with corresponding exceptional divisors e1,e2,. . .,en+1. When Shas a Bn-configuration, we call S a(rational) surface with a Bn-configuration (see Figure 2).

Whenx2,. . .,xn+1withxi=0, for alliare in general position (refer to Section 4 of [13] for definition), anyBn-exceptional system onSconsists of exceptional curves. Such a surface is called a Bn-surface. So a Bn-surface must have aBn-configuration.

Lemma 3.4. (i) Let S be a rational surface with a Bn-configuration. Then the Weyl group W(Bn) acts on all Bn-exceptional systems on Ssimply transitively.

(ii) Let S be a Bn-surface. Then the Weyl group W(Bn) acts on all Bn- configurations simply transitively.

Proof. It suffices to prove (i). Let (e1,e2,. . .,en+1) be a Bn-exceptional system on S. By Definition 3.3,ei =lσ(i)or flσ(i)fori=1, whereσis a permutation of{2,. . .,n+1}. Note that the Weyl group W(Bn) acts as the group generated by permutations of the npairs {(li, fli) | i=2,. . .,n+1}and interchanging ofli and fli in each pair (li, fli)i2. Then the result follows.

Let S(,Bn) be the moduli space of pairs (S,) where S is a Bn-surface (so the blown-up pointsx1=0,x2,. . .,xn+1are in general position), and ∈ | −KS|. DenoteMBn the moduli space of flat Bn bundles over . Then applying Corollary 3.2, we have the following identification.

Proposition 3.5. (i) S(,Bn) is embedded intoMBn as an open dense subset.

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(ii) Moreover, this embedding can be extended naturally to an isomorphism S(,Bn)∼=MBn,

by including all rational surfaces withBn-configurations.

Proof. The proof is similar to that inADEcases [13]. Firstly, we haveMBn ∼=c(Bn)⊗Z /W(Bn), andc(Bn)⊗Z/W(Bn)∼=H om((Bn),)/W(Bn) when we fixed the square root of unity ofJac()∼=. Refer to Section 3 of [13] for the detail.

Secondly, the restriction fromStoinduces a map (again denoted byφ) φ:S(,Bn)→H om((Bn),)/W(Bn).

This map is well defined; since by Lemma 3.4, choosing and fixing aBn-configuration on Sis equivalent to choosing and fixing a system of simple roots(Bn).

Thirdly, the mapφis injective. For this, we take a simple root system ofBnas β1= f−2l2 and βk=2αk+1 for 2≤kn.

Then the restriction induces an elementuH om((Bn),), which satisfies the following system of linear equations:

−2x2=p1,

2(xkxk+1)= pk, k=2,. . .,n,

where pi=u(βi). Obviously, the solution of this system of linear equations exists uniquely for given piwith 1≤in.

Finally, statement (ii) comes from Corollary 3.2 and the existence of the solutions to the above system of linear equations.

Remark. The situation here is very similar to that in the compactification theory of the moduli space of (projective)K3 surfaces. A natural question is how to extend the global Torelli theorem to the boundary components of a compactification (see, e.g. [11, 16]). If we consider the mapφ:S(,G)MG[13] forG=An,Dn, orEnas a type of period map, then the main result of [13] is a type of global Torelli theorem. And Proposition 3.5 implies that we can extend the theorem of Torelli type inDn+1case to a boundary component of the natural compactification.

In the following, we letS=Yn+1(x1,. . .,xn+1) be the blowup ofF1atn+1 points.

We can construct a Lie algebra bundle on S. Here we do not need the existence of

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the anticanonical curve . According to Section 2, we have a root system of Bn type, consisting of divisors on S:

R(Bn){±(f−2li), 2(lilj),±2(flilj) | i= j, 2i,jn+1}.

Thus, we can construct a Lie algebra bundle ofBn-type overS:

BnOn

DR(Bn)

O(D).

The fiberwise Lie algebra structure ofBnis defined as follows (the argument here is the same as that in [13]).

Fix the system of simple roots of Rnas

(Bn)= {α1= f−2l2,α2=2(l2l3),. . .,αn=2(lnln+1)},

and take a trivialization of Bn. Then over a trivializing open subset U,Bn|U ∼= U×(Cn

α∈RnCα). Take a Chevalley basis{xαU,αRn;hi, 1≤in}forBn|U and define the Lie algebra structure by the following four relations, namely, Serre’s relations on Chevalley basis (see [8], p. 147):

(a) [hihj]=0, 1≤i,jn.

(b) [hixαU]= α,αi xUα, 1≤in,αRn.

(c) [xUαx−αU ]=hαis aZ-linearly combination ofh1,. . .,hn.

(d) Ifα,βare independent roots, andβ,. . .,β+are theα-string through β, then [xUαxβU]=0 ifq=0, while [xαUxUβ]= ±(r+1)xα+βU ifα+βRn.

Note that hi, 1≤in are independent of any trivialization, so the relation (a) is always invariant under different trivializations. IfBn|V ∼=V×(Cn

α∈Rn) is another trivialization and fαU V is the transition function for the line bundleO(α)(αRn), that is, xαU= fαU VxαV, then the relation (b) is

hi

fαU VxαV = α,αi fαU VxαV, that is,

hixαV = α,αi xαV.

So (b) is also invariant. Relation (c) is also invariant since (fαU V)1 is the transition function forO(−α)(αRn). Finally, (d) is invariant since fαU VfβU Vis the transition function forO(α+β)(α,βRn).

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Therefore, the Lie algebra structure is compatible with the trivialization. Hence, it is well defined.

When the surfaceScontains as an anticanonical curve, restricting the above bundle to this anticanonical curve, we obtain a Lie algebra bundle of Bn-type over , which determines uniquely a flatBn bundle over. On the other hand, whenx1=0, we can identify these two line bundlesO(l1) andO(fl1) when restricting them to. Recall that the spinor bundlesS+n+1andSn+1 ofDn+1are defined as follows [12, 13] (here we omit the subscriptionn+1 for brevity):

S+=

D2=D·K=−1,D·f=1

O(D) and S=

T2=−2,T·K=0,T·f=1

O(T).

The identification of O(l1)∼=O(fl1) induces an identification of these two spinor bundlesS+andS, which is given by (of course, when restricted to)

S+O(−l1)∼=S.

From the representation theory, we know that this determines a flatBnbundle over. Conversely, ifS+|∼=S|, then we must have x1=0 (up to renumbering). For example, we consider then=2 case. Note that

S+|O(−(0))=OO((−x1x2)−(0))⊕O((−x1x3)−(0))⊕O((−x2x3)−(0)), S| =O((0)−(x1))⊕O((0)−(x2))⊕O((0)−(x3))⊕O(3(0)−(x1)−(x2)−(x3)).

Where for a point x, (x) means the divisor of degree one, andO((x)) means the line bundle determined by this divisor. Thus, S+O(−(0))=S implies that x1=0 (up to renumbering). The general case follows from similar arguments.

3.2 TheCnbundles

We take G=CnG=A2n1, where Cn=Sp(n) and A2n1=SU(2n). They satisfy the relationG=(G)Out(G).

LetS=Z2nbe a rational surface with anA2n1-configuration (see [13] or Figure 3) which contains as a smooth anticanonical curve. Recall [13] that Z2n is a (succes- sive) blowup ofF1at 2npointsx1,. . .,x2n on, with corresponding exceptional classes l1,. . .,l2n. Let fbe the class of fibers inF1, andsbe the section such that 0=sis the

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identity element of. The Picard group ofZ2nis H2(Z2n,Z), which is a lattice with basis s, f,l1,. . .,l2n. The canonical line bundleK= −(2s+3f2n

i=1li).

Recall that

P2n1:= {xH2(Z2n,Z)|x·K=x· f=x·s=0}

is a root lattice ofA2n1type. And we can take a simple root system of A2n1as (A2n1)= {αi =lili+1|1≤i≤2n−1}.

Note that [13] we have used the convention that2n

i=1xi =0.

Letρbe the generator ofOut(G)∼=Z2, such thatρ(αi)=α2nifori=1,. . ., 2n−1.

When the above simple root system is chosen, the pair (S,) determines a homo- morphismuH om((G),) which is given by the restriction map

u(α)=O(α)|.

Lemma 3.6. LetuH om((G),) be an element corresponding to a pair (S,), where Sis a surface with anA2n1-configuration. Thenρ·u=uif and only ifn(xi+x2n+1i)=0 fori=1,. . .,n.

Proof. Since u is the restriction map: αiO(αi)|,u(αi)=O(lili+1)|=xixi+1

for i=1,. . ., 2n−1. Hence, ρ·u=uu(αi)=u(α2ni)⇔xixi+1=x2nix2ni+1n(xi+x2ni+1)=0 since2n

i=1xi =0.

As in [13], we denote byS(,G) the moduli space ofG=A2n−1-surfaces with a fixed anticanonical curve, and byS(,G) the natural compactification by including all rational surfaces with A2n1-configurations. From [13], we know that there is an isomorphismφ:S(,G)−→ MG.

Corollary 3.7. For uMG→(MG)Out(G), φ1(u)∈S(,G) represents a class of sur- facesZ2n(x1,. . .,x2n) withxi+x2n+1−i =0 fori=1,. . .,n, and such a surface corresponds to a boundary point in the moduli space, that is,φ1(u)∈S(,G)\S(,G).

Proof. By Lemma 3.6, u∈(MG)Out(G) if and only if n(xi+x2n+1i)=0 fori=1,. . .,n.

There aren2connected components corresponding ton2points of ordernon. SinceMG is the component containing the trivialGbundle, we havexi+x2n+1i =0 fori=1,. . .,n.

Recall (Section 4 in [13]) that Z2n(x1,. . .,x2n)∈S(,G) if and only if 0,x1,. . .,x2n are in

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