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Quiver Variety

Klaus Altmann Lutz Hille

Abstract

Let Qbe a nite quiver without oriented cycles. Denote byU !M(Q) the ne moduli space of stable thin sincere representations ofQwith respect to the canonical stability notion.

We prove ExtlM(Q)(U U) = 0 for all l > 0 and compute the endomorphism algebra of the universal bundleU. Moreover, we obtain a necessary and sucient condition for when this algebra is isomorphic to the path algebra of the quiverQ. If so, then the bounded derived categories of nitely generated rightkQ-modules and that of coherent sheaves onM(Q) are related via the full and faithful functor;Ik QL U.

1 Introduction

(1.1)

LetQ be a quiver (i.e. an oriented graph) without oriented cycles denote byQ0 the vertices and byQ1 the arrows ofQ. For a xed dimension vectord, that is a mapd:Q0!ZZ 0, we denote by IH(d) :=f :Q0 !IR jPq2Q0 qdq = 0gthe vector space of the so-called weights with respect to d. We x an algebraically closed eld k. To each 2 IH(d) there exists the moduli spaceM (Qd) of -semistablek-representations ofQ with dimension vectord(cf. Ki]).

This space is known to be projective and, in case is in general position anddis indivisible, also smooth. Moreover, if we restrict ourselves to thin sincere representations, that is dq = 1 for all

q2Q

0, then M (Q) is also toric (cf. Hi2]). In any case, each integral weight induces an ample line bundle L( ) onM (Qd).

If is in general position and d indivisible, then M (Qd) is, in addition, a ne moduli space admitting a universal bundle U. The universal bundle splits into a direct sum of vector bundles

U =q2Q0Uq, and the summands Uq have rank dq (cf. Ki]). All known examples suggest that the universal bundles on those moduli spaces have no self-extensions, i.e. ExtMl (Qd)(UU) = 0 for alll>0. The issue of this paper is to prove this formula in special cases. The meaning of this property and its relation to tilting theory will be discussed in (1.4).

In this paper we restrict ourselves to thin sincere representations the corresponding moduli spaces are called toric quiver varieties. Because d = (1:::1) is xed, we will omit it in all notation introduced above. The direct summands of the universal bundle are line bundles, and they are characterized, up to a common twist, by the following property: For any arrow2Q1 pointing fromptoq(pq2Q0) the invertible sheaf Up;1Uqcorresponds to the divisor of all representations assigning the zero map to . Furthermore, there exists a distinguished weight c (see (1.2) and (2.7) for a denition and rst properties). We denote the corresponding moduli space byM(Q).

(1.2)

Polarized projective toric varieties may be constructed from lattice polytopes. If one wants to forget about the polarization, simply consider the inner normal fan of the polytope. In

x2 we give a detailed description of the moduli spaceM (Q) of thin sincere representations via its

\dening polytope" ( ). The easiest way to obtain ( ) from the quiver is to imagine as a

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one-way pipe system carrying liquid a weight 2IH describes the input (possibly negative) into the system at each knot. Using this language, ( ) is simply given as the set of all possible ows respecting both the direction of the pipes and the given input (see (2.3)).

Considering the opposite viewpoint, each ow through our pipe system requires a certain input, i.e.

a weight. In particular, from the special ow that is constant 1 at each pipe we obtain a special, so-called canonical, weight c. The corresponding ( c) is a reexive polytope (in the sense of Batyrev, Bat]), i.e. the moduli spaceM(Q) is Fano (Proposition (2.7)).

Fixing a weight in general position, i.e. M (Q) is smooth, ows and weights have still another meaning. Each ow denes an equivariant, with respect to the dening torus, eective divisor, and each weight 0 denes an element L( 0) in the Picard group ofM (Q). Assigning a ow its input weight corresponds to assigning a divisor its class in the Picard group (see (3.1)).

Example:

1) In the special case 0 := this recovers our ample line bundle introduced before.

2) The line bundleUp;1Uq corresponds to the weight with values 1 atp,;1 atq, and zero at all other points.

(1.3)

Our rst main result is Theorem (3.6) stating the lack of self-extensions ofU on the moduli space M(Q) with respect to the canonical weight, i.e. ExtlM(Q)(UU) = 0 for all l>0.

This is proved by using a slightly generalized Kodaira vanishing argument which works for toric varieties, cf. Theorem (3.5). As a Corollary of Theorem (3.6) we conclude that we obtain a full and faithful functor from the bounded derived category of nitely generated right modules over the endomorphism algebra Aof U into the bounded derived category of coherent sheaves on the moduli space M(Q) (Theorem (4.4)). Moreover, in Theorem (4.3) we provide a criterion for

A= EndM(Q)(UU) to be isomorphic to the path algebrakQof the quiverQ.

Combining both results we obtain the following relation between the derived categories of right

kQ-modules and of coherent sheaves onM(Q), respectively.

Theorem:

Assume Q is a quiver lacking (10)- and (tt)-walls (see (2.2) for an explanation).

Then,

;ILkQU :Db mod{kQ;!Db Coh;M(Q)

is a full and faithful functor from the bounded derived category of nitely generated rightkQ-modules into the bounded derived category of coherent sheaves on M(Q).

(1.4)

The result above is closely related to tilting theory. Since the fundamental paper Be], tilting theory has become a major tool in classifying vector bundles a tilting sheaf induces an equivalence of bounded derived categories, as in the previous Theorem. To be precise we recall the denition of a tilting sheaf (Bae]). A sheafT on a smooth projective variety is called a tilting sheaf if

1) it has no higher self-extensions, that is Extl(TT) = 0 for alll>0, 2) the direct summands generate the bounded derived category, and

3) the endomorphism algebraAofT has nite global (homological) dimension.

Then, the functorsIRHom(T;) and;ILAT dene mutually inverse equivalences of the bounded derived categories of coherent sheaves on the underlying variety ofT and of the nitely generated right A-modules, respectively. For constructions of tilting bundles and their relations to derived categories we refer to the following papers Ka], Be], Ru], Bo], and Or]. For the similar notion of a tilting module we refer to HR].

For our purpose, the notion of an exceptional sequence is more useful. LetCbe any of the categories introduced above: the category of nitely generated right modules over a nite dimensional algebra, the category of coherent sheaves on a smooth projective variety, or one of its derived categories.

Thus, C is either an abelian or a triangulated k-category. Each object in C has a unique, up to isomorphism and reordering, decomposition into indecomposable direct summands, i.e. is a

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Krull-Schmidt category. Moreover, the extension groups are dened and globally bounded they are nite-dimensionalk-vector spaces. An object inC is called exceptional if it has no self-extensions and its endomorphism ring is k. A sequence (E0:::En) of objects in Cis called exceptional if

1) each objectEi fori= 0:::nis exceptional and 2) Extl(EjEi) = 0 for alll0, andj>i.

Such a sequence is called strong exceptional if, additionally, 3) Extl(EiEj) = 0 for alll>0 and allij= 0:::n. Finally, it is called full if in addition to 1), 2) and 3)

4) the objectsEi fori= 0:::ngenerate the bounded derived category.

Thus, each full strong exceptional sequence denes a tilting bundleni=0Ei, because the endomor- phism algebra of ni=0Ei has global dimension at most n. Vice versa, each tilting bundle whose direct summands are line bundles gives rise to a strong exceptional sequence.

Using this language, our vanishing result Theorem (3.6) means that the direct summands of U form a strong exceptional sequence.

(1.5)

In general, this sequence cannot be full. Assume the contrary then the bounded derived categories in the previous theorem are equivalent. The rst one is a derived category of a hereditary abelian category, whose structure is well-known (Ri2]). In particular, the Serre functor (see BK] for the denition) coincides with the Auslander-Reiten translation and xes objects up to translation only in case the category is tame or just semi-simple (cf. Hap]x1.4/5). On the other hand, the Serre functor in the bounded derived category of coherent sheaves xes all skyscraper sheaves up to a translation. Consequently, an equivalence implies thatMis a point or a projective line in case the algebrakQis semi-simple or tame, respectively. It follows thatQis a point or the Kronecker quiver the remaining tame cases may not appear (see Ri1] Theorem p. 158).

Nevertheless, there is some hope that one may nd a complement U such thatUU is a tilting bundle. At least a class of very particular examples of tilting bundles on toric quiver varieties is known (Hi2], Theorem 3.9).

(1.6)

For an introduction to quivers and path algebras we refer the reader to Ri1] and ARS]

the theory of localizations may be found in S]. For an introduction to moduli spaces we mention N] and for moduli of representations of quivers we refer to the work of King Ki]. For results on triangulated categories we refer to Hap] and Har]. Our standard reference for toric geometry is Ke] for a short introduction to this area we also mention F].

We would like to thank G. Hein, A. King, and A. Schoeld for helpful discussions.

2 Moduli spaces of thin sincere representations

(2.1)

LetQbe a connected quiver without oriented cycles it consists of a setQ0of vertices, a setQ1of arrows, and two functionsst:Q1!Q0assigning to each arrow2Q1its sources() and its targett(). A representation ofQis a collection of nite dimensionalk-vector spacesx(q) for each vertexqtogether with a collection of linear mapsx() :x(s())!x(t()) for each arrow

2Q

1. The dimension vectord= (dq jq2Q0) of a representationxis dened bydq= dimx(q).

A representation is called thin if dimx(q) 1 for all q2 Q0 and sincere if dimx(q) 1 for all

q2Q

0. In this paper we consider only thin sincere representations.

We denote by R = 2Q1k the space of all thin sincere representations, that is x(q) = k. By

G = q2Q0k we denote the torus acting via conjugation on R. The orbits of this action are exactly the isomorphism classes of thin sincere representations, i.e. their moduli space may be

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obtained via GIT. Doing so, we have to deal with the notion of stability with respect to a given weight (cf. Ki]).

Denition:

The elements of the real vector space IH :=f :Q0!IRjPq2Q0 q = 0gare called weights of the quiver Q.

Let 2IH. A thin sincere representation x ofQis -stable (-semistable) if for each proper non- trivial subrepresentationy x we have Pq2Q0

jy(q)6=0 q <0 (0 respectively). Two semistable representationsxandyare calledS-equivalent with respect to if the factors of the stable Jordan- Holder ltration coincide.

A subquiver Q0 Q with Q00 =Q0 is -stable ( -semistable) if it has a -stable ( -semistable) representation. Two quivers are S-equivalent with respect to if they admit -semistable repre- sentations of the sameS-equivalence classes.

Finally, we denote by T( ) the set of all -semistable subtreesT QwithT0=Q0 and byQ1( ) the set of all arrowssuch thatQnfgis a -stable subquiver.

In other words, a representationxis -stable precisely when the subquiverQ0f2Q1jx()6= 0g is -stable. Moreover, a subquiver Q0 is -stable if and only if for all non-trivial proper subsets

S Q

0 which are closed under successors in Q0 we have Pq2S q < 0 (see Hi1] x2 and Hi2]

Lemma 1.4). We also note that each S-equivalence class contains a unique minimal -semistable subquiver { just take the disjoint union of the support of the Jordan-Holder factors.

(2.2)

As already mentioned in the beginning, for any given weight the moduli spaceM (Q) exists however, dierent weights may cause dierent moduli spaces. According to Hi1] there is a chamber system in IH, and the type ofM (Q) can only ip if crosses walls of the following type:

Denition:

W IH is called a (t+t;)-wall if

W =n 2IHj X

q2Q+0 q =; X

q2Q;0 q = 0o

for some decompositionQ0=Q+0tQ;0 such that the full subquiversQ+andQ;are both connected and such there are exactlyt+arrows pointing fromQ+0 toQ;0 andt;arrows the other way around.

We say that is in general position if does not lie on any wall and if the moduli space is not empty.

Assume is in general position, then M (Q) is smooth and has the (maximal) dimension d =

#Q1;#Q0+ 1, see Hi1]. Moreover, for those weights, every semistable thin sincere representation is stable.

(2.3)

To describe the toric structure ofM (Q) we introduce the real vector space of ows dened asIF :=fr:Q1!IR g=IRQ1. A ow is called regular if it has only non-negative values, i.e. if it respects the direction of the pipes. For any2Q1we denote byf2IF the characteristic ow mappingto 1 and keeping the remaining pipes dry. More generally, for each walkwwithout cycles in Qwe dene the characteristic ow fw mapping an arrow2w to 1, an arrow with

;1

2wto;1, and the remaining arrows to 0. This ow is regular if and only ifwis a path, i.e.

respects the orientation in Q.

There is a canonical linear map:IF !IH describing the input of ows if2Q1points from p to q, then(f) sendspandqonto 1 and;1, respectively. Thus

((r))q = X

s()=q

r; X t()=q

r:

This leads to the following denition:

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Denition:

The convex polytope of ows ( ) assigned to a weight is dened as the intersection ( ) :=;1( )\IRQ10:

This means that ( ) consists of exactly those regular ows respecting the prescribed input . Moreover, ( ) is compact sinceQhas no oriented cycles.

The vector spaces IF and IH contain the lattices IFZZ and IHZZ of integral ows and weights, respectively. For any integral weight :Q0!ZZ we dene the ane latticeM IF as the ber

IFZZ\;1( ), i.e.

M =nr2ZZQ1j X

s()=q

r; X t()=q

r= q for allq2Q0o: Any element r2M provides obviously an isomorphism (+r) :M:=M0;!M .

(2.4)

The following lemma will be crucial for the understanding of our ow polytope as well as for proving the upcoming vanishing theorem in x3 it explicitly provides points of the lattices

M . Let T Q be an arbitrary maximal tree. Each arrow 2T1 divides Q0 into two disjoint subsets, the sourceST() and the targetTT().

s s s

s s

s

s s

s

s s

s

s s

s

s

s - TT()

H

H;

;

S

S(

(

%

%

A

A(

(h

h

ST()

Lemma:

Fix a treeT and let 2IH. For any ow"there is a unique elementr=rT 2;1( )

IF satisfying r:="() for2=T1. Its remaining coordinates (i.e. for2T1) are given by

r ;"() = X

q2ST()q + X

TT()!ST()

"() ; X

ST()!TT()

"():

Proof:

First, we should note that both"and r are ows { the dierent notation for their coor- dinates ("() andr, respectively) was chosen for psychological reasons only. Now, let rbe some element of IF. If(r) = , then for any subdivisionQ0=Q+0 tQ;0 we obtain

X

s()2Q+0t()2Q;0

r; X s()2Q;0t()2Q+0

r= X

q2Q+0 q =; X

q2Q;0 q

just by summing up the M -equations withq2Q+0. The reverse implication is also true, even if we restrict ourselves to the special subdivisions provided by arrows 2T1 viaQ+0 :=ST() and

Q +

1 :=TT().

On the other hand, these subdivisions have the important property that is the only arrow that belongs to both the tree T and to one of the index sets fj s() 2 Q+0t() 2 Q;0g or

fjs()2Q;0t()2Q+0g. In particular, by just taking care of this single exception, in the above

equations we may always replacer by"(). 2

If the weight and the ow are integral, then so is r, i.e.r2M .

(2.5) Proposition:

Let 2IH be an integral weight, then the polytope of ows( ) M is always a lattice polytope. The associated projective toric variety equalsM (Q). Moreover, ( ) provides an ample, equivariant line bundle L( ) onM (Q).

(6)

Proof:

First, we establish a one-to-one correspondence between vertices of ( ) andS-equivalence classes of -semistable trees. Faces of ( ) in any dimension are obtained by forcing certain coordinates of IF to be zero. In particular, vertices are points with a maximal set of vanishing coordinates. Letr2( ) be a vertex and denote its support by

suppr:=f2Q1jr>0g:

If suppr contained any cycle of Q, then we could replace r by a dierent regular ow with the same weight and a smaller support. Hence, suppris contained in maximal trees ofQ. Moreover, we obtain that

every maximal treeT containing suppris -semistable, and

those trees are stable if and only if suppr=T1(which determines the tree uniquely).

To prove these facts, take a proper subsetQ+0 Q0that is closed under successors inT denoting

Q

;

0 :=Q0nQ+0 this means that there are no arrows pointing from Q+0 to Q;0 in T. Hence, using the formula mentioned in the previous proof,

X

q2Q+0 q =; X

Q;0!Q+0]

r 0:

Conversely, let T be any maximal tree. The previous lemma tells us that there is exactly one

r 2

;1( ) IF such that suppr T1 it has integer coordinatesr = PST() q for 2 T1. Moreover, ifT is -semistable, then these numbers are non-negative, meaning thatr2( ). Thus, it must be a vertex. Moreover, two dierent trees dene the same vertex if and only if they are

S-equivalent.

What does the inner normal fan ( ) look like? Denote byCthe matrix describing the incidences of our quiverC consists of #Q0rows and #Q1 columns, and forq2Q0,2Q1 we have

Cq:=

8

<

:

+1 ifq=s()

;1 ifq=t() 0 otherwise:

The free abelian group N :=ZZQ1=(C{rows) is dual to the lattice M :=M0 =;C{rows? IF. Hence, writing a2N for the images of the canonical vectorse2ZZQ1, we obtain

( ) =nha1:::aki Qnf1:::kgis the minimal element in someS-equivalence class of -semistable subquiverso:

According to Hi2], Theorem 1.7 and (3.3), this is exactly the fan dening the moduli spaceM (Q).

2

Example:

In the quiver below the canonical weight is c= (21;1;2).

s s

s A

A

A U

s

-

4

A

A

A U

1

2 3

C=

0

B

B

@

1 1 0 0 0

;1 0 1 1 0

0 ;1 ;1 0 1

0 0 0 ;1 ;1

1

C

C

A

The corresponding fan ( ), and the polytope ( c) look like the following:

(7)

s s

s s s

s s s s s s s

s s s s

;

;

;

; s s s s s

s

s

s

s

u

u

u u

u u

@

@

@

@

It is known that the toric variety of this fan is the blow up of the projective plane in two points, which is isomorphic to the blow up of the two-dimensional smooth quadric in one point.

(2.6)

Equivariant (with respect to the torus action), invertible sheaves Lon a toric variety

X( ) are completely determined by their order function ordL: (1) !ZZ or its piecewise linear continuation ordL:NIR!IR. Ifr()2Mprovides a local generatorxr()ofLonU() X( ), then ordL(a) is dened ashar()i ifa 2 (cf. Od]). Moreover, if L is an ample (or at least globally generated) invertible sheaf given by a lattice polytope MIR, then the local generators of L correspond to the vertices of . In particular, ordL(a) = minhai. Shifting the polytope by a vectorr 2M means to replace L byxrL. The corresponding order functions dier by the globally linear functionhri.

Lemma:

Let r 2 M be an arbitrary element. Then, the mapping a 7! ;r gives the order function of L( ) on M (Q). A di erent choice r0 2 M just changes the order function by the linear summand hr0;ri.

Proof:

We may user2M to carry ( ) into the \right" latticeM(see the end of (2.3)). Then, the order function applied toa2 ( )(1) NIR is

ordL( )(a) = minha( );ri= minhe( )i;r=;r: 2

(2.7)

Given the quiver Q, the canonical weight c announced in the introduction is dened as the weight of the ow rc that is constant 1 on every arrow. Explicitly, this means

c(q) := #farrows with sourceqg;#farrows with targetqg:

The advantage of c is the existence of a unique interior lattice point in the polytope ( c): it is again the owrc = 1:::1].

Proposition:

The polytope ( c) is reexive (in the sense of Bat]), its order function is;1 on the generators a2 ( c)(1), and the ample divisor L( c) is anti-canonical.

Proof:

The three claims are synonymous, i.e. we just have to look at the order function ofL( c).

Applying Lemma (2.6) onrc= 1 yields the result. 2

3 The cohomology of the universal bundle

(3.1)

From now on we assume that is an integral weight in general position, i.e.M (Q) is a smooth variety. To each integral ow we associate a divisor as follows:

f2IFZZ 7!D:=fx2M (Q)jx= 0g=

orb() ifa2 (1)=Q1( )

otherwise

(8)

with orb() denoting the closed orbit corresponding to the one-dimensional cone. One obtains surjective mapsIFZZ ;;!!DivM (Q) from the space of integral ows onto the equivariant divisors and, as a consequence, IHZZ ;;!!PicM (Q), 0 7!L( 0) from the integral weights to the Picard group (see also Hi2], Theorem 2.3). Applying the map:IFZZ ;;!!IHZZ means to assign a divisor its class in the Picard group.

Copying the denition of (2.3), every weight 0 gives rise to

( 0) :=fr2;1( 0)jr0 for 2Q1( )g:

Even if L( 0) is not ample onM (Q), the polytope ( 0) may still be used to describe the global sections:

Proposition:

The lattice points of( 0) provide a basis of the global sections ofL( 0). Moreover, if Q1( 0) Q1( ), then both polytopes ( 0) and ( 0) coincide.

Proof:

Given 0, we choose a owr2M 0 providing the order function of a divisor in the class dened by 0. The corresponding polytope of global sections is contained in M = M0 via the isomorphism (+r) :M0!M 0 it is mapped onto ( 0).

If Q1( 0) Q1( ), then ( 0) sits between ( 0) and fr 2;1( 0)jr 0 for2Q1( 0)g. On the other hand, Proposition (2.5) implies that the latter two polytopes are equal its proof shows quite directly that the inequalities parametrized byQ1nQ1( 0) are redundant for the denition of

( 0). 2

(3.2)

Since is in general position, there is a universal bundleU onM (Q) it splits into a direct sumU =q2Q0Uq of line bundles. The direct summandsUpq :=Up;1Uq ofEnd(U) have the following shape: Choose a walk from pto qalong (possibly reversed) arrows "1(1):::"m(m), i.e.1:::m2Q1and"(i)2f1g. Then, denoting byO() :=O(D) the sheaf corresponding to the prime divisorD,

Upq=Up;1Uq=Om

i=1

O(i)"(i):

In the Picard group ofM (Q) this sheaf does not depend on the particular choice of the walk from

ptoq: Using the language of (3.1), the sheavesiO(i)"(i)are induced from the owsPi"(i)fi, which all have the same weight.

Notation: Setting "(i) :="(i) and"() := 0 for2=f1:::mgprovides a function":Q1!

f1;10gfor every walk. This is the characteristic ow introduced in (2.3). Then, the sheafUpq

may be written asUpq =U(") =2Q1O()"() the corresponding weight pq:=(") has value 1 inp,;1 inq, and 0 in all other vertices.

(3.3) Proposition:

(1) Let 2 IHZZ be an integral weight in general position. Then, the sheaves UpqL( ) and

U

pq;1L( ) are generated by their global sections.

(2) If, additionally, = c, then the polytopes ( c pq) (describing the global sections) have the same dimension as( c).

Proof:

Since Uqp =Upq;1, it is sucient to consider the latter sheaf. The corresponding polytope ( ; pq) may be studied in dierent level sets:

( ; pq) = fr2;1( ; pq)jr0 for2Q1( )g

= fr2;1( )jr"() for2Q1( )g:

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