INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES
WARSZAWA 1998
ALMOST COMPLEX TORIC MANIFOLDS AND POSITIVE LINE BUNDLES
A K I O H A T T O R I
Department of Mathematics, Meiji University 1-1-1 Higashimita, Tama-ku, Kawasaki-shi, 214 Japan
E-mail: hattori@math.meiji.ac.jp
1. Introduction. Masuda [M] developed the theory of unitary toric manifolds which generalized the theory of toric varieties and the theory of Hamiltonian toral manifolds (toric manifolds) due to Delzant [D] in some direction. There are works of Karshon and Tolman [KT] and of Grossberg and Karshon [GK] in a similar direction. An advantage of Masuda’s theory is the introduction of the notion of multi-fan attached to unitary toric manifolds. The multi-fan is essentially a simplicial complex with some extra data and equipped with a map from the set of its vertices to the second homology group H 2 (BT ; Z) of the classifying space BT of the torus T acting on the manifold.
One of the main results of [M] is the multiplicity formula which relates the index of the Dirac operator twisted by a line bundle L acted on by the torus T to some data coming from the moment map of the bundle. Similar formulas are also in [KT] and [GK].
The moment map is a T -invariant map from M into the second cohomology with real coefficients H 2 (BT, R). Irreducible representations of a torus T are one dimensional.
They form an abelian multiplicative group Hom(T, S 1 ). We identify Hom(T, S 1 ) with H 2 (BT, Z). So, if χ is a virtual representation of T then it can be written as
χ = X
u∈H
2(BT ,Z)
m(u)χ u , m(u) ∈ Z,
where χ u is the irreducible representation corresponding to u. The multiplicity formula identifies the integer m(u) with the value d 0 L (u) of a degree function d 0 L defined on H 2 (BT, R) minus a union of certain affine hyperplanes when χ is the index of the Dirac operator D L twisted by the line bundle L.
In this paper we shall deal with almost complex toric manifolds satisfying some mild conditions. Given a T -line bundle we define a piecewise linear map Ψ L from the realization of the first barycentric subdivision of the simplicial complex attached to the multi-fan
1991 Mathematics Subject Classification: 57S25, 58F05.
The paper is in final form and no version of it will be published elsewhere.
[95]
into H 2 (BT, R) such that its image is contained in the union of hyperplanes described above. Theorem 3.5, work done jointly with Masuda, states that the winding number d ¯ L (u) of the map Ψ L around u ∈ H 2 (BT, R) coincides with the value d L (u) of the degree function d L which is intimately related to d 0 L . The same sort of statement (Theorem 3.11) holds also for the degree function of [KT]. This allows us to express the multiplicity m(u) purely in terms of the multi-fan and algebraic data of the line bundle L.
We shall also define a notion of positiveness of line bundles in such a way that ana- logues of the Nakai criterion and the Kodaira vanishing theorem hold (Corollary 4.8 and Theorem 4.21; also see Theorem 4.19). Furthermore, it is shown (Theorem 5.4) that if the Todd genus of the manifold is equal to 1, then the above definition of positiveness is quite parallel to the classical convexity criterion of ample line bundles in the theory of toric varieties, cf. e.g. [F],[O].
The organization of the paper is as follows. In Section 2 we review Masuda’s theory in a way suitable to our purpose. Section 3 is devoted to the results surrounding the map Ψ.
In Section 4 we introduce the notion of positiveness of line bundles and give proof of the analogues of the Nakai criterion and the Kodaira vanishing theorem. In proving the Nakai criterion a formula in Theorem 4.2 which expresses the number c 1 (L) n [M ] in terms of the degree function ¯ d L is crucial. For the proof of Theorem 4.2 we use a combinatorial formula (Lemma 4.5) concerning the volume of rational polytopes. The formula is a simple one but seems to be new. In the last section, Section 5, the case where the Todd genus equals 1 will be dealt with.
The author would like to thank M. Masuda for stimulating conversations and coop- eration.
2. Almost complex toric manifolds and multi-fan. A closed, connected 2n- dimensional almost complex manifold M acted on by a torus T will be called an almost complex toric manifold if the following conditions are satisfied.
1. The action preserves the almost complex structure.
2. If T 0 denotes the trivializer of the action, then dim T /T 0 = n.
3. The fixed point set of the action (which we denote by M T ) is not empty.
We set T = T /T 0 . T acts effectively on M , and M T is an isolated set.
According to [M] a closed, connected codimension 2 submanifold M i of M will be called a characteristic submanifold if it is a fixed point set component of a certain subcircle S i of T and M i ∩ M T 6= ∅. M i inherits the almost complex structure from M . Let Σ 0 M denote the set of all indices i of characteristic submanifolds M i . We set
Σ k−1 M = {I = {i 1 , i 2 , . . . i k }; M I = M i
1∩ · · · ∩ M i
k6= ∅, i ν ∈ Σ 0 M }.
Then Σ 0 M , Σ 1 M , . . . , Σ n−1 M form a simplicial set Σ M (in [M] this simplicial set was denoted by Γ M ). Note that all M I are also almost complex toric manifolds. In the sequel we shall make the following assumption.
All M I are connected and M I ∩ M T 6= ∅.
(2.1)
The assumption implies in particular M I is a point of M T for any (n−1)-simplex I ∈ Σ n−1 M .
Let ν i be the normal bundle of M i in M . It is a complex line bundle. Denoting by f i : M i → M the inclusion map we define ξ i ∈ H 2
T (M ; Z) by ξ i = f i∗ (1) where f i∗ : H 0
T (M ; Z) → H 2
T (M ; Z) is the Gysin homomorphism of f i . If p ∈ M i ∩ M T , then ν i |p is an irreducible T module, that is, ν i |p ∈ Hom(T , S 1 ). The restriction of ν i |p to S i
does not depend on the choice of p in M i ∩ M T .
Hom(T , S 1 ) is an abelian multiplicative group. We shall identify it with H 2 (BT ; Z) by the isomorphism Hom(T , S 1 ) → H 2 (BT ; Z) given by α 7→ c T 1 (α), where c T 1 is the equivariant first Chern class. The T -module corresponding to u ∈ H 2 (BT ; Z) is denoted by χ u . For example, ν i |p = χ ξ
i|p .
Lemma 2.1 ([M], Lemma 1.3). Take I ∈ Σ n−1 M and p ∈ M I . Then the set {ξ i |p, i ∈ I}
forms a basis of H 2 (BT ; Z). In particular , ξ i |p is a primitive element.
In a similar way there is a standard isomorphism between Hom(S 1 , T ) and H 2 (BT ; Z).
The embedding S i ,→ T determines a primitive element of H 2 (BT ; Z) up to sign and hence a primitive element v i ∈ H 2 (BT ; Z) up to sign. The sign will be determined by requiring
< ξ i |p, v i >= 1
where < > is the coupling between cohomology and homology. It follows easily that {v i ; i ∈ I} is the dual basis of {ξ i |p, i ∈ I}. The following lemma will play an important role in the sequel.
Lemma 2.2 ([M], Lemma 1.5). There is an identity
u = X
i∈Σ
0M< u, v i > ξ i ∈ ˆ H T 2 (M ; R)
which holds for any u ∈ H 2 (BT ; R). Here ˆ H 2
T (M ; R) is the degree 2 part of H ∗
T (M ; R)/S- torsion where S is the multiplicative set generated by non-zero elements in H 2 (BT ; R).
The simplicial set Σ M is equipped with a projection map π : Σ 0 M → H 2 (BT ; Z) defined by π(i) = v i . It induces a piecewise affine map π : |Σ M | → H 2 (BT ; R), where |Σ M | is the realization of Σ M . We shall denote by s I the realization of I ∈ Σ M in |Σ M |. For each I, π maps s I injectively on the affine simplex s 0 I in H 2 (BT ; R) spanned by {v i ; i ∈ I}.
Once an orientation of H 2 (BT ; R) is fixed, each (n − 1)-simplex s 0 I (I ∈ Σ n−1 M ) will be given the orientation o I defined in the following way. Fix i ∈ I. The vector v i intersects s 0 I transversally. Requiring the positive orientation of the vector v i followed by o I should coincide with the given orientation of H 2 (BT ; R) determines o I . This does not depend on the choice of i ∈ I.
Lemma 2.3. |Σ M | is a closed pseudo-manifold. This means that every simplex is con- tained in some (n − 1)-dimensional simplex , and , for each J ∈ Σ n−2 M , s J is the face of precisely two (n − 1)-simplices s I and s I
0. Moreover , if an orientation of H 2 (BT ; R) is fixed and each (n − 1)-simplex s I is oriented so that π|s I : s I → s 0 I preserves the orienta- tion, then P s I is the fundamental class of |Σ M |. This means that , if |Σ M | = S
ν |Σ M | ν
is the decomposition into connected component of |Σ M |, then P
s
I⊂|Σ
M|
νs I generates
H n−1 (|Σ M | ν ; Z) for each ν.
P r o o f. Take J ∈ Σ n−2 M . By virtue of (2.1) M J is a connected almost complex sub- manifold of dimension 2 on which the torus T acts non-trivially so that it is complex projective line and has precisely two fixed points M I and M I
0. This means that I and I 0 are only simplices to which J is incident, namely s J is the face of s I and s I
0. Moreover Masuda showed ([M], Lemma 4.4) that s I and s I
0lie on different sides of s I ∩ s I
0. This implies that π|s I ∪ s I
0is injective and hence the orientability of |Σ M |.
Lemma 2.4. The degree of π : |Σ M | → H 2 (BT ; R) \ {0} is equal to T [M ], the Todd genus of M .
This is essentially a restatement of [M], Theorem 4.2 paraphrased by using the pro- jection π.
Lemma 2.5 ([M], Lemma 3.2). The equivariant first Chern class c T 1 (L) of a complex T -line bundle L over M can be written in the form
c T 1 (L) = X
c i ξ i ∈ ˆ H T 2 (M ; Z).
Note. [M], Lemma 3.2 shows also that every element in ˆ H 2
T (M ; Z) is of the form c T 1 (L). Similarly every element of ˆ H 2
T (M ; R) can be written in the form P c i ξ i with c i ∈ R.
For a complex T -line bundle L with c T 1 (L) = P c i ξ i ∈ ˆ H 2
T (M ; Z), we define the affine hyperplane F i in H 2 (BT ; R) by
F i = {u ∈ H 2 (BT ; R); < u, v i >= c i }.
We set F I = T
i∈I F i for I ∈ Σ k−1 M . F I is a point for I ∈ Σ n−1 M .
The moment map Φ L of L is a T -invariant map Φ L : M → H 2 (BT ; R) uniquely determined by the complex T -line bundle L. It has the following properties.
Lemma 2.6 ([M], Lemma 6.5). Φ L (M I ) ⊂ F I for any I ∈ Σ k−1 M . We shall add the following assumption:
All isotropy subgroups of the T action are subtori , and each fixed point set component of subtori contains a point in M T .
With this assumption the quotient space M/T becomes a compact, connected ori- entable manifold of dimension n with boundary. The boundary ∂(M/T ) is S M i /T . Since the moment map Φ L is T -invariant it factors through the map ¯ Φ L : M/T → H 2 (BT ; R).
Using this map ¯ Φ L , the degree function
d L : H 2 (BT ; R) \ [
F i → Z
is defined as follows. Choose an orientation o(T ) of the torus T , and define the orienta- tion o(M/T ) of M/T by requiring that o(T ) followed by o(M/T ) should coincide with (−1) n(n−1)/2 times that of M as an almost complex manifold. The orientation o(T ) also determines that of H 2 (BT ; R). Take u ∈ H 2 (BT ; R) \ S F i . Then d L (u) is the degree of
H n (M/T, ∂(M/T ); Z) → H n (H 2 (BT ; R), H 2 (BT ; R) \ {u}; Z).
This definition does not depend on the choice of o(T ).
The function d L is locally constant. There is a transition formula for the values of d L when one moves from a component to another. Components of H 2 (BT ; R) \ S F i
will be called chambers. Two chambers W α and W β are called adjacent if W α ∩ W β has dimension n − 1. In this case, let F i be such that W α ∩ W β ⊂ F i . Then W α ∩ W β is the closure of a component W αβ of F i \ S
F
i6=F
jF j . W αβ will be called a wall between W α
and W β . Note that there may be F j with j 6= i, j ∈ Σ 0 M but F j = F i . The transition formula is stated in the following way.
Lemma 2.7 ([KT], Remark 6.5; [M], Lemma 6.9). Let W α and W β be adjacent cham- bers. Take points u α ∈ W α and u β ∈ W β such that the segment u α u β from u α to u β
crosses the wall W αβ transversally. Then d L (u α ) = d L (u β ) + X
F
i⊃W
αβsign < u β − u α , v i > d L|M
i(u αβi ), where u αβi = u α u β ∩ F i .
Here d L|M
ihas to be understood as follows. Let S i be the subcircle which stabilizes points in M i as before. Set T i = T /S i . Then T i acts effectively on M i . Take a point p ∈ M i ∩ M T and put γ = c i ξ i |p ∈ Hom(T , S 1 ). The restriction of γ to Hom(S i , S 1 ) does not depend on the choice of p in M i ∩ M T , and S i acts trivially on Lχ −γ |M i . Hence Lχ −γ |M i can be regarded as a T i -line bundle, and d Lχ
−γ|M
iis defined. If u lies in F i \ S
j6=i F j we define
d L|M
i(u) = d Lχ
−γ|M
i(u − γ).
Note that u − γ is in H 2 (BT i ; R). It is easy to show that d L|M
i(u) is well-defined inde- pendently of the choice of p.
Lemma 2.8 ([M], Theorem 3.1). Let K = V n
T ∗ M be the canonical line bundle of M . The equivariant Chern class of K considered as an element of ˆ H T 2 ¯ (M ; Z) is given by
c T 1 (L) = − X
ξ i ∈ ˆ H T 2 ¯ (M ; Z).
Define Φ 0 L : M → H 2 (BT ; R) by
Φ 0 L = Φ L − 1 2 Φ K . For each i ∈ Σ 0 M the affine hyperplane F i 0 is defined by
F i 0 = {u ∈ H 2 (BT ; R); < u, v i >= c i + 1/2}.
From 2.6 and 2.8 it follows that Φ 0 L (M i ) is contained in F i 0 . The degree function d 0 L : H 2 (BT ; R) \ [
F i 0 → Z
is defined by using Φ 0 L in a similar way as d L . Note that H 2 (BT ; Z) is contained in H 2 (BT ; R) \ S F i 0 .
We are now in a position to state the main result of [M]. Once a T -invariant metric
on M and a T -invariant U (1)-connection of L are given, the Dirac operator D L of the
almost complex manifold M twisted by the line bundle L is defined. Its index, ind D L ,
is a T -module. In the topological context it is expressed as the image π ∗ (L) of L by the
Gysin homomorphism π ∗ : K T (M ) → K T (pt) = R(T ), where R(T ) is the character ring of T . It is identified with the group ring of Hom(T , S 1 ) over Z.
Theorem 2.9 ([M], Theorem 7.2; [KT], Theorem 2). If we write ind D L as ind D L = X
u∈H
2(BT ;Z)
m(u)χ u , then m(u) = d 0 L (u).
This finishes the review of [M].
3. Map Ψ. As we saw in the previous section the degree function d L was defined by using the moment map of L. It is desirable to explain it by using only combinatorial data of the simplicial set Σ M and the numbers c i associated with i ∈ Σ 0 M which describe the T -line bundle L. The aim of this section is to give such an explanation. This is a joint work with Masuda. The results can be extended to cover unitary toric manifolds. So we will only give statement of results and sketch of proof here leaving the details elsewhere.
Let Σ 0 M be the first barycentric subdivision of Σ M and S M = |Σ 0 M | the realization of Σ 0 M . The barycenter of I ∈ Σ k−1 M is denoted by b I . These barycenters form the set of vertices of Σ 0 M . A simplex of Σ 0 M is of the form
(b I
1, b I
2, . . . , b I
l) with I 1 ⊂ I 2 ⊂ . . . ⊂ I l .
The realization of (b I
1, . . . , b I
l) in S M will be denoted by |b I
1, . . . , b I
l|. For each I ∈ Σ k−1 M we set
σ I = [
I
1=I
|b I
1, . . . , b I
l| ⊂ S M
It is called the dual cell of I ∈ Σ k−1 M . When I = {i} ∈ Σ 0 M we simply write σ i for σ I . We see that σ I ⊂ σ J if I ⊃ J . Also, if I ∩ I 0 = ∅ and I ∪ I 0 is a simplex of Σ M , then σ I ∩ σ I
0= σ I∪I
0. The set of all dual cells {σ I } stratifies the complex S M . In particular
S M = [
i∈Σ
0Mσ i .
Let Lk Σ
MI be the link of I in S M for I ∈ Σ k−1 M . It is a simplicial set whose vertices are those j ∈ Σ 0 M such that j 6∈ I and {j} ∪ I ∈ Σ k M , and whose simplices are those J ∈ Σ l−1 M such that I ∩ J = ∅ and I ∪ J ∈ Σ k+l−1 M .
Lemma 3.1. The boundary ∂σ I of the dual cell σ I is the realization of a simplicial set isomorphic to the first barycentric subdivision Lk Σ 0
M
I of Lk Σ
MI.
P r o o f. The boundary is the realization of a simplicial set Σ(I) whose simplices are those (b I
1, . . . , b I
l) with I ⊂ I 1 but I 6= I 1 and I 1 ⊂ · · · ⊂ I l . The correspondence which sends each simplex (b J
1, . . . , b J
l) of Lk Σ 0
M
I into (b I∪J
1, . . . , b I∪J
l) is an isomorphism of simplicial sets between Lk Σ 0
MI and Σ(I).
Lemma 3.2. The simplicial set Lk Σ
MI is isomorphic to Σ M
Ifor any I ∈ Σ k−1 M . P r o o f. Take i ∈ Lk 0 M I. Then M I,i = M I ∩ M i is a characteristic submanifold of M I
by virtue of the assumption (2.1). The vertex map from Lk 0 M I to Σ 0 M
I
which sends i into
(I, i) gives the desired isomorphism.
As an immediate corollary of Lemmas 3.1 and 3.2 we obtain Corollary 3.3. ∂σ I is homeomorphic to S M
I.
Given a collection ˆ c = {c i } indexed by Σ 0 M we define a map Ψ c ˆ : S M → H 2 (BT ; R)
in the following way. It will be affine on each simplex |b I
1, . . . , b I
l| of S M . Hence it is sufficient to assign a value for each vertex b I . We do this by descending induction on the dimension k − 1 of I ∈ Σ k−1 M . When k = n, Ψ ˆ c (b I ) is determined by the equation
< Ψ ˆ c (b I ), v i >= c i for i ∈ I.
Note that {v i ; i ∈ I} is a basis of H 2 (BT ; Z) by Lemma 2.1. For I ∈ Σ k−1 M with 0 < k < n we set C I = {J ∈ Σ k M ; I ⊂ J } and define
Ψ ˆ c (b I ) = 1
#C I
X
J ∈C
IΨ ˆ c (b J ),
where #C I is the cardinality of C I . The affine hyperplanes F i and F I are defined in a similar manner as in Section 2. As a direct consequence of the definition we have:
Lemma 3.4. Ψ ˆ c (σ I ) ⊂ F I for any I ∈ Σ k−1 M . In particular Ψ c ˆ (S M ) ⊂ S F i .
Let u be a point in H 2 (BT ; R) \ S F i . We define ¯ d c ˆ (u) ∈ Z as the degree of the homomorphism
Ψ c∗ ˆ : H n−1 (S M ; Z) → H n−1 (H 2 (BT ; R) \ {u}; Z).
Note that a preferred orientation of H 2 (BT ; R) determines those of S M and H 2 (BT ; R) simultaneously. Thus ¯ d ˆ c (u) is defined independently of the choice of orientations of H 2 (BT ; R). When ˆ c comes from a T -line bundle L, i.e. when
c T 1 (L) = X
c i ξ i ∈ ˆ H 2
T (M ; Z) we write ¯ d L for ¯ d ˆ c .
Theorem 3.5. The function ¯ d L : H 2 (BT ; R) \ S F i → Z coincides with d L .
Before proceeding to the proof we shall make some comments concerning the function d ¯ ˆ c . At this point and hereafter we shall identify ˆ c = {c i } with the cohomology class ˆ
c = P
i c i ξ i ∈ ˆ H 2
T (M ; R).
Given an element γ ∈ H 2 (BT ; R) we put ˆ
c γ = {c 0 i } with c 0 i = c i − < γ, v i >
and
F i γ = {u; < u, v i >= c 0 i }.
for each i. The translation by −γ sends the hyperplane F i to F i γ .
Assertion 3.6. If we regard ˆ c = P c i ξ i and ˆ c γ = P c 0 i ξ i as elements in ˆ H 2
T (M ; R), then ˆ c γ = ˆ c − γ. If u is in H 2 (BT ; R) \ S F i , then u − γ is in H 2 (BT ; R) \ S F i γ , and
d ¯ ˆ c (u) = ¯ d ˆ c
γ(u − γ).
P r o o f. By Lemma 2.2, γ = P < γ, v i > ξ i as elements in ˆ H 2
T (M ; R). Hence ˆ
c − γ = X
(c i − < γ, v i >)ξ i = ˆ c γ .
Then it is easy to see that that Ψ ˆ c
γis the composition of Ψ ˆ c and the translation by −γ.
The identity above for the degree function ¯ d ˆ c follows readily from this observation.
Take i ∈ Σ 0 M and take a vector γ in F i . Then F i γ is identified with H 2 (BT i ; R) ⊂ H 2 (BT ; R). We set
ˆ
c γ
i|M i = {c 0 j ; j ∈ Σ M
i},
and define Ψ ˆ c
γi|M
i: S M
i→ H 2 (BT i ; R) as before. From this the degree function d ¯ ˆ c
γi|M
i: H 2 (BT i ; R) \ [
j∈Σ
MiH 2 (BT i ; R) ∩ F j γ → Z
is induced as before.
Assertion 3.7. If we regard ˆ c as an element of ˆ H 2
T (M ; R) then ˆ c γ
i|M i is nothing but the restriction of ˆ c γ to M i . In particular , in case ˆ c comes from a T -line bundle L and γ lies in H 2 (BT ; Z) ∩ F i , ˆ c γ
i|M i coincides with ¯ d Lχ
−γ|M
i.
P r o o f. We see that ξ j |M i = 0 if M i ∩ M j = ∅ by definition of ξ j . Hence ˆ
c|M i = X
j∈Lk
0ΣM
{i}
c j ξ j |M i + c i ξ i |M i .
Moreover ξ j |M i belongs to ˆ H 2
T
i(M i ; Z) ⊂ ˆ H 2
T (M i ; Z) because M i ∩ M j is a characteristic submanifold of M i for j ∈ Lk 0 Σ
M
{i} under the assumption (2.1).
On the other hand, by Lemma 2.2
γ = X
j∈Lk
0ΣM
{i}
< γ, v j > ξ j |M i + < γ, v i > ξ i |M i .
Since < γ, v i >= c i we obtain ˆ
c γ
i|M i = ˆ c|M i − γ = X
j∈Lk
0ΣM
{i}
(c j − < γ, v j >)ξ j |M i = X
j∈Lk
0ΣM