The Serre Duality for Holomorphic Vector Bundles over Strongly Pseudo Convex CR Manifolds
Mitsuhiro Itoh
Institute of Mathematics, University of Tsukuba, Japan e-mail: [email protected]
(2000 Mathematics Subject Classification : 53C40, 53C15. )
1 Main Theorem.
1.1 The Serre duality for a holomorphic vector bundleEand its dual vector bundle E∗ holds over a compact, strongly pseudo convex CR manifold. This duality is a vector bundle generalization of the Serre duality for scalar valued harmonic forms over a strongly pseudo convex CR manifold given by N. Tanaka.
LetM be a compact, strongly pseudo convex CR (2n−1)-dimensional manifold andE be a holomorphic vector bundle overM. Assume 2n−1≥5 in what follows.
Then we have
Theorem A([I-S]). LetHp,q(M;E) be the space ofE-valued harmonic (p, q)-forms overM. Then
Hp,q(M;E)∼=Hn−p,n−q−1(M;E∗) (1.1)
for any (p, q), 0≤p≤n, 0≤q≤n−1. HereE∗ is the dual ofE.
TheoremB([I-S]). Theq-th cohomology groupHq(M;E⊗ΛpTˆM∗) satisfies Hq(M;E⊗ΛpTˆM∗)∼=Hn−q−1(M;E∗⊗Λn−pTˆM∗)
(1.2)
for any (p, q), 0 ≤ p ≤ n, 0 ≤ q ≤ n−1. Here ˆTM is the holomorphic tangent bundle of M and Hq(M;F) denotes the ∂-cohomology group of the ∂-complex {Cq(M;F);∂=∂q}associated with a holomorphic vector bundleF.
Moreover,
Hq(M;E)∼=Hn−q−1(M;E∗⊗KˆM), 0≤q≤n−1, (1.3)
where ˆKM = ΛnTˆM∗ denotes the canonical complex line bundle ofM.
1.2 Over a compact complex n-dimensional complex manifold M the following duality
Hq(Mn; Ωp(F))∼=Hn−q(M; Ωn−p(F∗)) (1.4)
17
holds for a holomorphic vector bundle F and 0≤ p, q ≤n, where Ωp(F) denotes the sheaf of holomorphic F-valued p-forms. This is called Serre duality due to J.P. Serre ([S]), which is a fundamental machinery in study of the ∂-cohomology of holomorphic vector bundles over a complex manifold. See for this [K] and also [O-S-S], for examples.
1.3 In his famous lecture note [T] N.Tanaka established the following duality over a strongly pseudo convex CR manifold in scalar valued harmonic (p, q)-forms:
Hp,q(M)∼=Hn−p,n−q−1(M), (1.5)
for any (p, q), 0≤p≤n, 0 ≤q≤n−1. Here Hp,q(M) is the space of harmonic (p, q)-forms onM.
2 Strongly Pseudo Convex CR Manifolds
2.1 Let M be a (2n−1)-dimensional manifold. If M carries the following CR structure (S, θ, P, I, g), we callM orM with (S, θ, P, I, g) a strongly pseudo convex CR manifold (by abbrevation, s.p.c. CR manifold);
(i) θ is a contact form of M so that P is a subbundle of T M defined by P = Kerθ,
(ii) S is a complex subbundle of the tangent vector bundleTCM such that S∩S={0},
and
[Γ(S),Γ(S)]⊂Γ(S) (2.6)
(iii) Further
PC=S⊕S
andI is an endomorphism ofP satisfyingI2=−idP and S={X∈PC|IX=−√
−1X}
(iv) The symmetric bilinear form, called Levi form,g:P×P −→ R g(X, Y) =−dθ(IX, Y)
(2.7)
is positive definite. So the Levi form g together with the contact form θ yields a smooth Riemannian metrich=g⊕θ⊗θonM.
Since a s.p.c. CR manifold M is contact, M admits a smooth vector field ξ, called basic field ( or Reeb field).
We call a s.p.c. CR manifold normal, when it holds [ξ,Γ(S)]⊂Γ(S).
(2.8)
2.2 Example 1. The following are typical examples of s.p.c. CR manifolds.
(a) a strictly convex real hypersurfaceM in a complex manifoldN, (b) a Sasakian manifold,
(c) anS1-bundle over a complex Hodge manifold,
(d) link of zero locus of a complex weighted homogenious polynomial f(z1,· · ·, zn+1) =X
ci1i2···in+1z1a1· · ·zn+1an+1, namely, the linkKf is defined
Kf =S2n+1∩ {z∈Cn+1|f(z) = 0}.
(2.9)
Notice that examples (b), (c) and (d) are normal s.p.c. manifolds
3 Holomorphic Vector Bundles
3.1 LetE −→M be a complex vector bundle over a s.p.c. CR manifoldM. Definition. A holomorphic structure of E is a first order differential operator
∂=∂E : Γ(M;E)−→Γ(M;E⊗S∗) satisfying (i) ∂(f u) =f ∂(u) +u⊗d”f, (3.10)
(hered” denotes the CR operator, that is, theS-component of the ordinary exterior derivatived), namely, if we set∂X(u) =∂(u)(X),X∈S, then, equivalently
(i0) ∂X(f u) =f ∂X(u) +Xf u, (3.11)
and
(ii) ∂X∂Yu−∂Y∂Xu−∂[X,Y]u= 0, (3.12)
u∈Γ(M;E) and X, Y are smooth sections ofS. We call the bundle (E, ∂), orE holomorphic.
The condition (ii) means the vanishing of (0,2)-component of the curvature formRD, whenE admits a connectionD whose (0,1)-part is the operator∂.
A smooth sectionuofE is calledholomorphicwhen it satisfies∂u= 0.
3.2 Example 2. The quotient complex vector bundle ˆTM =TCM/SofTCM is holomorphic. It is called the holomorphic tangent bundle of M, whenM is s.p.c.
CR. The holomorphic structure∂ is defined
∂Xu=π([X, Z]), (3.13)
where Z is a section of TCM such that π(Z) = u and π : TCM −→ TˆM is the projection.
Notice. IfM is normal, then the basic fieldξ, more preciselyπ(ξ), is a holomor- phic section of ˆTM
3.3 Similarly to holomorphic vector bundles over a complex manifold, we have the following basic facts.
The tensor product E ⊗F of holomorphic vector bundles E and F over a s.p.c. CR manifold is also holomorphic. Moreover the dual bundle E∗ and the exterior product bundle ΛkE are holomorphic. Furthermore, ifU is a holomorphic subbundle of a holomorphic vector bundleE, then it induces the quotient bundle E/U which is holomorphic;
0 −→ U −→ E −→ E/U −→ 0 (3.14)
Example 3. Let E −→M be a holomorphic vector bundle over a Hodge manifold M andM be a s.p.c. CR manifold whose CR structure comes from theS1-bundle overM. Then it is not hard to show that the pull-back ofEoverM is holomorphic.
Example 4. If M is a s.p.c. CR manifold M which is a real hypersurface in a complex manifoldM, then any holomorphic vector bundleE overM restricts toM holomorphic.
Notice that if dimM ≥7, any holomorphic vector bundleE over a s.p.c. CR manifold fulfills the local holomorphic frame property, i.e., around any point ofM Eadmits a local holomorphic frame (s1,· · ·, sr). It still open whether this property holds even when dim≤5.
4 Cohomologies Hp,q(M;E)
4.1 Let E be a holomorphic vector bundle over a s.p.c. CR manifold M. We define a complex{Cq(M;E);∂=∂q}, called the∂-complex as follows: Cq(M;E) = Γ(M;E⊗ΛqS∗),q= 0,1,· · ·n−1 and the operator∂q : Cq(M;E)−→ Cq+1(M;E) by
(∂q ϕ)(Y1,· · ·, Yq+1) (4.15)
= X
j
(−1)j+1∂Y
j(ϕ(Y1,· · · ,Yˆj,· · · , Yq+1))
+ X
i,j
(−1)i+jϕ([Yi, Yj], Y1,· · ·,Yˆi,· · ·,Yˆj,· · ·, Yq+1),
whereϕ∈ Cq(M;E), Yj ∈Γ(M;S), j= 1,· · · , q+ 1.
It holds
∂q+1◦∂q= 0.
(4.16)
Hence we have the cohomology groupHq(M;E),q= 0,· · ·, n−1 as Hq(M;E) = Ker∂q/Im∂q−1.
(4.17)
4.2 To define the (p, q)-cohomology group Hp,q(M;E) we take the holomorphic vector bundle E⊗Λp( ˆTM∗) by tensoring E with the holomorphic exterior product bundle Λp( ˆTM∗), and byCp,q(M;E) we denote Γ(M;E⊗ΛpTˆM∗ ⊗ΛqS∗), the space of all smooth sections ofE⊗ΛpTˆM∗ ⊗ΛqS∗.
Notice that in our terminology Cq(M;E) =C0,q(M;E). Further ˆTM ∼=Cξ⊕S as a smooth complex vector bundle so that ˆTM∗ ∼=Cθ⊕S∗ and
ΛpTˆM∗ ∼=Cθ⊗Λp−1S∗⊕ΛpSp. (4.18)
Definition. The (p, q)-cohomologyHp,q(M;E) is defined Hp,q(M;E) =Hq(M;E⊗ΛpTˆM∗).
(4.19)
5 HarmonicE-valued (p, q)-forms
5.1 LetM be, same as before, a s.p.c. CR manifold. ThenM admits the canonical volume formdv=θ∧(dθ)n−1and also the Riemannian metrich=g⊕θ⊗θinduced from the Levi formg and the contact formθofM.
In order to get the notion of harmonic forms taking values in E⊗ΛpTˆM∗ we need to define the formal adjoint∂∗ of the operator∂q =∂. For this, just like the complex manifold case as in [K-M], we define the Hodge star operator
] : E⊗ΛpTˆM∗ ⊗ΛqS∗ −→E∗⊗Λn−pTˆM∗ ⊗Λn−q−1S∗, (5.20)
defined byψ−→](ψ) =∗ψ, by exploiting the identification (18). Then the formal adjoint∂∗ is defined
∂∗= (−1)n−k]∗◦∂◦] (5.21)
onE⊗ΛpTˆM∗ ⊗ΛqS∗,k=p+q. It is not difficult to show that∂∗ is theL2-adjoint of the holomorphic operator∂:
h∂ϕ, ψi=hϕ, ∂∗ψi (5.22)
forϕ∈ Cp,q(M;E) andψ∈ Cp,q+1(M;E∗). The inner product is hϕ, ψi=
Z
M
(ϕ, ψ)dv.
A sectionϕofCp,q(M;E) is calledharmonicwhen it satisfies (∂∗∂+∂∂∗)ϕ= 0
(5.23)
and denote byHp,q(M;E) the space of allE-valued harmonic (p, q)-forms.
5.2 By Kohn’s theorem([K]), if dimM ≥5, thenHp,q(M;E) is finite dimensional andCp,q(M;E) is endowed with the Hodge-decomposition property in terms of the Laplace operator ∂∗∂+∂∂∗, (for the details, see [T], or the original paper [K]), so that we get the first part of TheoremB from TheoremA.
Proof of Theorem A. Let ψ be an element of Hp,q(M;E). Then we have by definition
∂Eψ= 0, and ∂∗Eψ= 0.
Sinceψ∈ Cq(M;E⊗ΛpTˆM∗),
] ψ∈ Cn−q−1(M;E∗⊗Λn−pTˆM∗).
(5.24)
Note that ]ψis anE∗-valued form.
Then by exploiting the definition of the formal adjoint, we have
∂E∗(]ψ) = (−1)n−k ](∂E)∗ψ= 0, wherek=p+qand
∂∗E∗(]ψ) = (−1)n−k ] ∂E]∗(]ψ) = (−1)n−k ] ∂Eψ= 0.
Thus, we have
]ψ∈Hn−p,n−q−1(M;E∗) (5.25)
and from that]∗=]−1, ]induces the isomorphism ]:Hp,q(M;E)−→Hn−p,n−q−1(M;E∗) (5.26)
to obtain TheoremA.
6 Remarks
6.1 To show the last half part of TheoremB, we observe the following.
Hq(M;E) ∼= H0,q(M;E) (6.27)
∼= Hn,n−q−1(M;E∗)
∼= H0,n−q−1(M; ΛnTˆM∗ ⊗E∗)
∼= Hn−q−1(M; ΛnTˆM∗ ⊗E∗), which is justHn−q−1(M;E∗⊗KˆM).
6.2 LetM be a s.p.c. CR (2n−1)-dimensional manifold which is normal and ξ be a basic field ofM. Thenξ is a holomorphic section of the holomorphic tangent bundle ˆTM which vanishes nowhere.
Then this fieldξinduces the inner product which satisfies for α∈ Cq(M;E⊗ΛpTˆM∗) = Γ(M;E⊗ΛpTˆM∗ ⊗ΛqS∗)
∂ iξα=iξ ∂α (6.28)
so that this induces a linear map between the cohomology groups:
iξ : Hp,q(M;E)−→Hp−1,q(M;E) : [ψ] 7→ [iξψ]
(6.29) which fullfils
iξ◦iξ = 0.
(6.30)
6.3 Example 5 Let M = Kf be a link of zero locus in C4 of the weighted homogeneous polynomialf =z16+z62+z63+z24. Then dimM = 5 and the weight of f is (1,1,1,3) and the degree d= 6. So the Hodge numbers are h2,0(M) = 1 and h1,1(M) = 19 by computing in terms of the Milnor algebra associated to the f, wherehp,q(M) = dimCHp,q(M). See [I] for the counting formula of hp,q(M).
By applying the Serre duality in the trivial bundle case,M admits a non-trivial holomorphic 3-formψ, sinceH0(M; Λ3TˆM∗)∼=C. This is because
h2,0=h0,2=h3,0= dimCH3,0(M).
Here the second equality is from the Serre duality and then H3,0(M)∼=H0(M; Λ3TˆM∗).
Moreover iξψ ∈ H0(M; Λ2TˆM∗) is a holomorphic 2-form on M which is also non-trivial so that this form yields a base ofH2,0(M)∼=C.
References
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