# Wednesday, January 27 ## Bundles and Connections :::{.definition title="Connections"} Let \( \mathcal{E}\to X \) be a vector bundle, then a **connection** on \( \mathcal{E} \) is a map of sheaves of abelian groups \[ \nabla: \mathcal{E}\to \mathcal{E}\tensor \Omega^1_X \] satisfying the *Leibniz rule*: \[ \nabla (fs) = f \nabla s + s\tensor ds \] for all opens $U$ with $f\in \OO(U)$ and $s\in \mathcal{E}(U)$. Note that this works in the category of complex manifolds, in which case $\nabla$ is referred to as a **holomorphic connection**. ::: :::{.remark} A connection $\nabla$ induces a map \[ \tilde{\nabla}: \mathcal{E}\tensor \Omega^p &\to \mathcal{E}\tensor \Omega^{p+1} \\ s \otimes \omega &\mapsto \nabla s \wedge w + s\tensor d \omega .\] where $\wedge: \Omega^p \tensor \Omega^1 \to \Omega^{p+1}$. The standard example is \[ d: \OO &\to \Omega^1 \\ f &\mapsto df .\] where the induced map is the usual de Rham differential. ::: :::{.exercise title="?"} Prove that the *curvature* of $\nabla$, i.e. the map \[ F_{\nabla} \da \nabla \circ \nabla: \mathcal{E}\to \mathcal{E}\tensor \Omega^2 \] is $\OO\dash$linear, so $F_{\nabla}(fs) = f\nabla \circ \nabla(s)$. Use the fact that $\nabla s \in \mathcal{E}\tensor \Omega^1$ and \( \omega \in \Omega^p \) and so \( \nabla s \otimes \omega \in \mathcal{E} \Omega^1 \otimes \Omega^p \) and thus reassociating the tensor product yields $\nabla s \wedge \omega \in \mathcal{E}\tensor \Omega^{p+1}$. ::: :::{.remark} Why is this called a connection? \begin{tikzpicture} \fontsize{25pt}{1em} \node (node_one) at (0,0) { \import{/home/zack/SparkleShare/github.com/Notes/Class_Notes/2021/Spring/FourManifolds/sections/figures}{2021-01-27_14-05.pdf_tex} }; \end{tikzpicture} This gives us a way to transport $v\in \mathcal{E}_p$ over a path \( \gamma \) in the base, and $\nabla$ provides a differential equation (a flow equation) to solve that lifts this path. Solving this is referred to as **parallel transport**. This works by pairing \( \gamma'(t) \in T_{ \gamma(t) } X \) with \( \Omega^1 \), yielding \( \nabla s = ( \gamma'(t)) = s( \gamma(t)) \) which are sections of \( \gamma \). Note that taking a different path yields an endpoint in the same fiber but potentially at a different point, and $F_\nabla = 0$ if and only if the parallel transport from $p$ to $q$ depends only on the homotopy class of \( \gamma \). > Note: this works for any bundle, so can become confusing in Riemannian geometry when all of the bundles taken are tangent bundles! ::: :::{.example title="A classic example"} The Levi-Cevita connection $\nabla^{LC}$ on $TX$, which depends on a metric $g$. Taking $X=S^2$ and $g$ is the round metric, there is nonzero curvature: \begin{tikzpicture} \fontsize{45pt}{1em} \node (node_one) at (0,0) { \import{/home/zack/SparkleShare/github.com/Notes/Class_Notes/2021/Spring/FourManifolds/sections/figures}{2021-01-27_14-15.pdf_tex} }; \end{tikzpicture} In general, every such transport will be rotation by some vector, and the angle is given by the area of the enclosed region. ::: :::{.definition title="Flat Connection and Flat Sections"} A connection is **flat** if $F_\nabla = 0$. A section \( s \in \mathcal{E}(U) \) is **flat** if it is given by \[ L(U) \da \ts{ s\in \mathcal{E}(U) \st \nabla s = 0} .\] ::: :::{.exercise title="?"} Show that if $\nabla$ is flat then $L$ is a *local system*: a sheaf that assigns to any sufficiently small open set a vector space of fixed dimension. An example is the constant sheaf $\ul{\CC^d}$. Furthermore $\rk(L) = \rk(\mathcal{E})$. ::: :::{.remark} Given a local system, we can construct a vector bundle whose transition functions are the same as those of the local system, e.g. for vector bundles this is a fixed matrix, and in general these will be constant transition functions. Equivalently, we can take $L\tensor_\RR \OO$, and $L\tensor 1$ form flat sections of a connection. ::: ## Sheaf Cohomology :::{.definition title="Čech complex"} Let \( \mathcal{F} \) be a sheaf of abelian groups on a topological space $X$, and let \( \mathfrak{U} \da \ts{U_i} \covers X \) be an open cover of $X$. Let $U_{i_1, \cdots, i_p} \da U_{i_1} \intersect U_{i_2} \intersect\cdots \intersect U_{i_p}$. Then the **Čech Complex** is defined as \[ C_{\mathfrak{U}}^p(X, \mathcal{F}) \da \prod_{i_1 < \cdots < i_p} \mathcal{F}(U_{i_1, \cdots, i_p}) \] with a differential \[ \bd^p: C_{\mathfrak{U}}^p(X, \mathcal{F}) &\to C_{\mathfrak{U}}^{p+1}(X \mathcal{F}) \\ \sigma &\mapsto (\bd \sigma)_{i_0, \cdots, i_p} \da \prod_j (-1)^j \ro{\sigma_{i_0, \cdots, \hat{i_j}, \cdots, i_p}}{U_{i_0, \cdots, i_p}} \] where we've defined this just on one given term in the product, i.e. a $p\dash$fold intersection. ::: :::{.exercise title="?"} Check that $\bd^2 = 0$. ::: :::{.remark} The Čech cohomology $H^p_{\mathfrak{U}}(X, \mathcal{F})$ with respect to the cover \( \mathfrak{U} \) is defined as $\ker \bd^p/\im \bd^{p-1}$. It is a difficult theorem, but we write $H^p(X, \mathcal{F})$ for the Čech cohomology for any sufficiently refined open cover when $X$ is assumed paracompact. ::: :::{.example title="?"} Consider $S^1$ and the constant sheaf $\ul{\ZZ}$: \begin{tikzpicture} \fontsize{42pt}{1em} \node (node_one) at (0,0) { \import{/home/zack/SparkleShare/github.com/Notes/Class_Notes/2021/Spring/FourManifolds/sections/figures}{2021-01-27_14-40.pdf_tex} }; \end{tikzpicture} ere we have \[ C^0(S^1, \ul{\ZZ}) = \ul{\ZZ}(U_1) \oplus \ul{\ZZ}(U_2) = \ul{\ZZ} \oplus \ul{\ZZ} ,\] and \[ C^1(S^1, \ZZ) = \bigoplus_{\substack{ \text{double} \\ \text{intersections}} } \ul{\ZZ}(U_{ij}) \ul{\ZZ}(U_{12}) = \ul{\ZZ}(U_1 \intersect U_{2}) = \ul{\ZZ} \oplus \ul{\ZZ} .\] We then get \[ C^0(S^1, \ul{\ZZ}) &\mapsvia{\bd} C^1(S^1, \ul{\ZZ}) \\ \ZZ \oplus \ZZ &\to \ZZ\oplus \ZZ \\ (a, b) &\mapsto (a-b, a-b) ,\] Which yields $H^*(S^1, \ul{\ZZ}) = [\ZZ, \ZZ, 0, \cdots]$. :::