[Math] The classifying space of a gauge group

at.algebraic-topologyclassifying-spacesgauge-theorygroup-actions

Let $G$ be a Lie group and $P \to M$ a principal $G$-bundle over a closed Riemann surface. The gauge group $\mathcal{G}$ is defined by

$$\mathcal{G}=\lbrace f : P \to G \mid f(p \cdot g) = g^{-1}f(p)g\ (\forall g \in G, p \in P) \rbrace.$$

I want to understand the following statement which I found in Atiyah-Bott (Roy. Soc. London Ser. A 308).

PROPOSITION 2.4. Let $BG$ be the classifying space for $G$. Then in homotopy theory
$$B\mathcal{G} = \mathrm{Map}_P(M,BG).$$ Here the subscript $P$
denotes the component of a map of $M$ into $BG$ which induces $P$.

This is proved by showing that $\pi:\mathrm{Map}_G(P,EG) \to \mathrm{Map}_P(M,BG)$ is a universal $\mathcal{G}$-bundle.

My questions:

  1. Why is $\mathrm{Map}_G(P,EG)$ contractible?
  2. How do we see that $\pi:\mathrm{Map}_G(P,EG) \to \mathrm{Map}_P(M,BG)$ is locally trivial? Here for a $G$-equivariant map $f:P \to EG$, $\pi(f)$ is the map $P/G \to EG/G$ which is canonically induced by $f$.

Notes:

  • It is easy to see that $\mathrm{Map}(P,EG)$ is contractible, because $EG$ is contractible. But, because of the $G$-actions, it does not seem that we can apply the same discussion to $\mathrm{Map}_G(P,EG)$.

  • For the second question, Atiyah and Bott say the following. But I can not understand it and I want to understand the details.

    If $BG$ is paracompact and locally contractible, which is easily arranged, $\pi$ will be a locally trivial principal fibring, as follows easily from the homotopy properties of fibrings.

  • If there is a good exposition of this problem, please let me know.

Best Answer

Proof of (1):

(a). Suppose $X$ and $Y$ are $G$-spaces, the action of $G$ on $X$ is free, and $X\to X/G$ is a principal bundle, then the space of $G$-equivariant maps $$ F(X,Y)^G $$ is the same thing as the space of sections of the fibration $X\times_G Y \to X/G$.

(b). If $E\to B$ is a Hurewicz fibration, with $B$ connected and the fiber contractible, then the space of sections is again contractible. This can be seen as follows: the adjunction property shows that $$ \text{sec}(E \to B) \to F(B,E) \to F(B,B) $$ is a fibration (the displayed fiber is the space of sections---it's the fiber over the basepoint of $F(B,B)$ given by the identity map of $B$---and the other two spaces are function spaces). Since $F$ is contractible the map $E\to B$ is a homotopy equivalence and therefore so is $F(B,E) \to F(B,B)$. Hence $\text{sec}(E\to B)$ is contractible.

(c). It follows from (a) and (b) that the space of sections of $X\times_G Y \to X/G$ is contractible whenever $Y$ is.

(d). In your case, $X = P$ and $Y = EG$. Hence, $F(P,EG)^G$ is contractible.

Proof of (2):

I'll prove something slightly less, which is enough for what you wish to have:

I claim that if $X \to X/G$ and $Y \to Y/G$ are principal $G$-bundles then the map $$ F(X,Y)^G \to F(X/G,Y/G) $$ is a Hurewicz fibration. This is the same thing as the map $$ \text{sec}(X\times_G Y\to X/G) \to \text{sec}(X/G\times Y/G\to X/G) $$ induced by the fibration $X\times_G Y \to X/G \times Y/G$.

This map of section spaces is the map of fibers which is induced by a map of fibrations over a common base space: the first fibration is $F(X/G, X\times_G Y) \to F(X/G,X/G)$ and the second one is $F(X/G, X/G\times Y/G) \to F(X/G,X/G)$. Since the map $F(X/G, X\times_G Y) \to F(X/G, X/G\times Y/G)$ is a fibration, it is formal to show that the map of section spaces is too.

In your situation we take $X = P$ and $Y = EG$. Then we see that the map $$ F(P,EG)^G \to F(P/G,BG) $$ is a fibration. The fiber at the point of $F(P/G,BG)$ defined by the classifying map for $P \to P/G$ is then your gauge group $\cal G$.

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