nLab Dolbeault complex

Contents

Context

Complex geometry

Differential geometry

synthetic differential geometry

Introductions

from point-set topology to differentiable manifolds

geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry

Differentials

V-manifolds

smooth space

Tangency

The magic algebraic facts

Theorems

Axiomatics

cohesion

infinitesimal cohesion

tangent cohesion

differential cohesion

graded differential cohesion

singular cohesion

id ⊣ id ∨ ∨ fermionic ⇉ ⊣ ⇝ bosonic ⊥ ⊥ bosonic ⇝ ⊣ Rh rheonomic ∨ ∨ reduced ℜ ⊣ ℑ infinitesimal ⊥ ⊥ infinitesimal ℑ ⊣ & étale ∨ ∨ cohesive ʃ ⊣ ♭ discrete ⊥ ⊥ discrete ♭ ⊣ ♯ continuous ∨ ∨ ∅ ⊣ * \array{ && id &\dashv& id \\ && \vee && \vee \\ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \\ && \bot && \bot \\ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& \mathrm{R}\!\!\mathrm{h} & \stackrel{rheonomic}{} \\ && \vee && \vee \\ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \\ && \bot && \bot \\ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \\ && \vee && \vee \\ &\stackrel{cohesive}{}& \esh &\dashv& \flat & \stackrel{discrete}{} \\ && \bot && \bot \\ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \\ && \vee && \vee \\ && \emptyset &\dashv& \ast }

Models

Lie theory, ∞-Lie theory

differential equations, variational calculus

Chern-Weil theory, ∞-Chern-Weil theory

Cartan geometry (super, higher)

Contents

Idea

The Dolbeault complex is the analog of the de Rham complex in complex geometry.

Definition

Dolbeault complex

On a complex manifold XX the de Rham complex Ω •(X)\Omega^\bullet(X) refines to a bigraded complex Ω •,•(X)\Omega^{\bullet, \bullet}(X), where a differential form of bidegree (p,q)(p,q) has holomorphic degree pp and antiholomorphic degree qq, hence is given on a local coordinate chart by an expression of the form

ω=∑f IJdz i 1∧⋯∧dz i p∧dz¯ j 1∧⋯∧dz¯ j q. \omega = \sum f_{I J} d z_{i_1} \wedge \cdots \wedge d z_{i_p} \wedge d \bar z_{j_1} \wedge \cdots \wedge d \bar z_{j_q} \,.

Moreover, the de Rham differential d\mathbf{d} decomposes as

d=∂+∂¯, \mathbf{d} = \partial + \bar \partial \,,

where ∂:Ω •,•→Ω •+1,•\partial \colon \Omega^{\bullet, \bullet}\to \Omega^{\bullet + 1, \bullet} and ∂¯:Ω •,•→Ω •,•+1\bar \partial \colon \Omega^{\bullet, \bullet}\to \Omega^{\bullet, \bullet + 1}.

The Dolbeault complex of XX is the chain complex (Ω •,•(X),∂¯)(\Omega^{\bullet, \bullet}(X), \bar \partial). The Dolbeault cohomology of XX is the cochain cohomology of this complex.

Holomorphic differential forms

Here Ω p,0(X)\Omega^{p,0}(X) defines a holomorphic vector bundle and a holomorphic section is a differential form with local expression as above, such that the coefficient functions f IJf_{I J} are holomorphic functions. This is called a holomorphic differential form.

For p<dim ℂ(X)p \lt dim_{\mathbb{C}}(X) equivalently this is a differential form in the kernel of the antiholomorphic Dolbeault operator ∂¯\bar \partial.

Properties

Dolbeault theorem

The complex analog of the de Rham theorem is the Dolbeault theorem:

for XX a complex manifold then its Dolbeault cohomology in bi-degree (p,q)(p,q) is naturally isomorphic to the abelian sheaf cohomology in degree qq of the abelian sheaf Ω p≔Ω p,0\Omega^p \coloneqq \Omega^{p,0} of holomorphic p-forms

H p,q(X)≃H q(X,Ω p). H^{p,q}(X)\simeq H^q(X,\Omega^p) \,.

(…)

Let Disk complDisk_{compl} be the category of complex polydiscs in ℂ n\mathbb{C}^n and holomorphic functions between them.

For p∈ℕp \in \mathbb{N} write Ω p:Disk complex op→Set\Omega^p \colon Disk_{complex}^{op} \to Set for the sheaf of holomorphic differential p-forms.

Proposition

For XX a complex manifold, let {U i→X}\{U_i \to X\} be a holomorphic good open cover. Then the Cech cohomology of this cover with coefficients in Ω p\Omega^p in degree qq is the Dolbeault cohomology in bidegree (p,q)(p,q)

H p,q(X)≃π 0sPSh(Disk comp)(C({U i},Ω p[q])). H^{p,q}(X) \simeq \pi_0 sPSh(Disk_{comp})(C(\{U_i\}, \Omega^p[q])) \,.

For instance (Maddock, theorem 1.0.1).

On Stein manifolds

Proposition

(Cartan theorem B)

For XX a Stein manifold,

H k(Ω p,•(X),∂¯)={0 k≠0 Ω hol p(X) k=0. H^k(\Omega^{p,\bullet}(X), \bar \partial) = \left\{ \array{ 0 & k \neq 0 \\ \Omega^p_{hol}(X) & k = 0 } \right. \,.

For instance (Gunning-Rossi).

Proposition

For XX a Stein manifold of complex dimension nn, the compactly supported Dolbeault cohomology is

H k(Ω c p,•(X),∂¯)={0, k≠n (Ω hol n−p(X)) *, H^k(\Omega_c^{p, \bullet}(X), \bar \partial) = \left\{ \array{ 0 , & k \neq n \\ (\Omega_{hol}^{n-p}(X))^\ast } \right. \,,

where on the right (−) *(-)^\ast denotes the continuous linear dual.

First noticed in (Serre).

Todd genus

By the Hirzebruch-Riemann-Roch theorem the index of the Dolbeault operator is the Todd genus.

Relation to Spin cSpin^c-structures

A complex manifold, being in particular an almost complex manifold, carries a canonical spin^c structure. The corresponding Spin^c Dirac operator identifies with the Dolbeault operator under the identification of the spinor bundle with that of holomorphic differential forms

S(X)≃∧ 0,•T *X. S(X) \simeq \wedge^{0,\bullet} T^\ast X \,.

References

A formal geometry version:

Last revised on October 18, 2023 at 05:59:23. See the history of this page for a list of all contributions to it.