Algebraic de Rham Cohomology and Gauss–Manin Connections
Table of Contents
In this note, we discuss algebraic de Rham cohomology and related concepts. The purpose of this note is not to give a very detailed account of the theorems and concepts, but provide a surface level overview. The reason I wanted to write about this is because I want to learn about de Rham–Witt cohomology, for which this is a prerequisite. I have not found a reference that I am completely satisfied with, but a lot of my sources come from Dustin Clausen’s notes.
Algebraic de Rham Cohomology
The de Rham cohomology originated from smooth manifolds, where $\mathrm H^k_{\mathrm{dR}}(M)$ is the cohomology of the de Rham complex $\Omega^{\bullet}(M)$.
There is a different version where the isomorphism is between de Rham cohomology and singular cohomology $\mathrm H^k_{\mathrm{dR}}(M)\cong\mathrm H^k(M,\underline{\mathbb R})$, for which the map is induced by the chain morphism
$$\omega\mapsto \left(\sigma\mapsto \int_{\sigma}\omega\right)$$its well-definedness is exactly the statement of Stokes theorem.
We want a version of this for algebraic varieties.
For any scheme $X/S$, define the hypercohomology
$$\mathrm{H}_{\mathrm{dR}}^n(X)=\mathbb H^n(X,\Omega^\bullet_X)$$as the algebraic de Rham cohomology of $X$.
For algebraic varieties (or even complex manifolds), we do not have an adequate partitions of unity, so we can have $\Omega^p$ not acyclic. Hypercohomology captures the higher sheaf cohomology $\mathrm{H}^q(X,\Omega^p)$ when $\Omega^p$ is not necessarily acyclic. This is captured in
$$E_1^{p,q}=\mathrm{H}^q(X,\Omega^p)\Rightarrow \mathrm{H}^{p+q}_{\mathrm{dR}}(X)$$which is called the Hodge-to-de Rham spectral sequence. For smooth affine $X$, we know that $\Omega_X^p$ is acyclic, so one could compute de Rham cohomology easily with $H^n(\Omega^\bullet_X)$. Grothendieck proved an analogue of de Rham’s theorem for complex algebraic varieties.
Gauss–Manin Connection
Recall that a connection on a vector bundle $\mathcal E$ on a scheme $X$ is a map $\nabla:\mathcal E\rightarrow \mathcal E\otimes_{\mathcal O_X}\Omega^1_X$ satisfying Leibniz rule
$$\nabla(U)(fe)=e\otimes \mathrm df+f\nabla(U)(e)$$where $f\in\mathcal O_X$ and $e\in\mathcal E(U)$ and $U\subseteq X$ an open. For each derivation $D\in \mathcal{Der}_k(\mathcal O_X,\mathcal O_X)\cong \mathcal{Hom}_{\mathcal O_X}(\Omega_X^1, \mathcal O_X)$, define $\nabla_D:\mathcal E\rightarrow\mathcal E$
$$\nabla_D:\mathcal E\xrightarrow{\nabla}\mathcal E\otimes_{\mathcal O_X}\Omega^1_X\xrightarrow{\mathrm{id}\otimes D}\mathcal E\otimes_{\mathcal O_X} \mathcal O_X\cong \mathcal E$$which we call the covariant derivative in the direction $D$. We can extend the connection to a map $\nabla:\mathcal E\otimes\Omega^p_X\rightarrow \mathcal E\otimes\Omega^{p+1}_X$ by
$$\nabla(s\otimes\omega)=\nabla(s)\land\omega+s\otimes \mathrm dw$$then the curvature is $\nabla^2:\mathcal E\rightarrow\mathcal E\otimes_{\mathcal O_X}\Omega^2_X$. Recall that a connection is called flat or integrable if the curvature $\nabla^2=0$.
Let $f:X\rightarrow S$ be a smooth proper morphism of smooth schemes over field $k$ of characteristic $0$. The Gauss–Manin connection is the canonical flat connection on the relative de Rham cohomology sheaves
$$\nabla_{\mathrm{GM}}:\mathcal H^n_{\mathrm{dR}}(X/S)\longrightarrow \mathcal H^n_{\mathrm{dR}}(X/S)\otimes \Omega^1_{S/k}$$where $\mathcal H^n_{\mathrm{dR}}(X/S)=\mathrm{R}^nf_{*}\Omega_{X/S}^\bullet$. They are constructed in the following way: consider the exact sequence
$$0\to f^*\Omega^1_{S/k}\to\Omega^1_{X/k}\to \Omega^1_{X/S}\to 0$$which induces a Gauss–Manin filtration $\mathrm{Fil}^p\,\Omega^\bullet_X$ defined by
$$\mathrm{Fil}^p\,\Omega^n_X=\mathrm{Im}\left(f^*\Omega^p_{S/k}\otimes_{\mathcal O_X}\Omega^{n-p}_{X/k}\xrightarrow{\eta\otimes\alpha\mapsto f^*\eta\wedge \alpha}\Omega^n_{X/k}\right)$$then consider the exact sequence
$$0\to f^*\Omega^1_{S/k}\otimes_{\mathcal O_X}\Omega^\bullet_{X/S}[-1]\to \Omega^\bullet_{X/k}/\mathrm{Fil}^2\,\Omega^\bullet_{X/k}\to \Omega^\bullet_{X/S}\to 0$$In the derived category we have a connecting morphism
$$\Omega^\bullet_{X/S}\longrightarrow f^*\Omega^1_{S/k}\otimes_{\mathcal O_X}\Omega^\bullet_{X/S}$$applying derived pushforward
$$\mathrm{R}f_*\Omega^\bullet_{X/S}\longrightarrow \mathrm{R}f_*\left(f^*\Omega^1_{S/k}\otimes_{\mathcal O_X}\Omega^\bullet_{X/S}\right)$$By the projection formula
$$\mathrm{R}f_*\left(f^*\Omega^1_{S/k}\otimes_{\mathcal O_X}\Omega^\bullet_{X/S}\right)\cong \mathrm{R}f_*\Omega^\bullet_{X/S}\otimes_{\mathcal O_S}\Omega^1_{S/k}$$Therefore we have a morphism
$$\mathrm{R}f_*\Omega^\bullet_{X/S}\longrightarrow \mathrm{R}f_*\Omega^\bullet_{X/S}\otimes_{\mathcal O_S}\Omega^1_{S/k}$$taking cohomology sheaves gives us
$$\nabla_{\mathrm{GM}}:\mathcal H^n_{\mathrm{dR}}(X/S)\longrightarrow \mathcal H^n_{\mathrm{dR}}(X/S)\otimes_{\mathcal O_S}\Omega^1_{S/k}$$which is the Gauss–Manin connection.
References
- [BT82]Raoul Bott and Loring W. Tu. Differential Forms in Algebraic Topology. Graduate Texts in Mathematics. Vol. 82. Springer-Verlag. New York. 1982.
- [Bre97]Glen E. Bredon. Sheaf Theory. Graduate Texts in Mathematics. Vol. 170. Springer-Verlag. New York. 1997.