kakarotyjn said:
Thank you quasar,but I'm sorry I still can't understand the connection between the way we construct E and the transition functiong_{\alpha \beta}.In E, (x,y) is equivalent to (x,g_{\alpha \beta} by definition.But how does this equivalent relation induce that g_{\alpha \beta} is the transition function?Why there is an equivalent relation?
In order to prove g_{\alpha \beta} is the transition function,we need to find fiber-preserving homeomorphisms \psi_\alpha and \psi_\beta for g_{\alpha \beta}(x)=\psi_\alpha \psi_\beta^{-1}
Thank you very much!
Mmh, maybe your problem stems from the technicalities of the definition. Because strictly speaking it is not true that in E, (x,y) is equivalent to (x,g_{\alpha \beta}y). Because E is obtained by quotienting a
disjoint union over the index alpha. This means that the elements of E are actually equivalences classes of elements of the form ((x,\alpha),y) where ((x',\beta),y') is identified to ((x,\alpha),y) iff x'=x and y'=g_{\alpha \beta}y.
So what we're doing here is we're constructing E by taking a covering {U_\alpha} of the base B and considering the trivial bundles U_{\alpha}\times F over each U_\alpha. Then we glue all of these trivial bundles along fibers over the points where they "intersect" (i.e. over the intersections U_{\alpha}\cap U_{\beta}) by using homeomorphisms coming from the action G\rightarrow \mathrm{Homeo}(F) of the group G on F. This induces a potential "twisting" in the bundle.
For instance, the Mobius bundle can be constructed in this way using G=Z/2Z-->{±Id
R} and a covering of S
1 of only two open sets {U
1,U
2}. Then the intersection of U
1 and U
2 has two connected components. On the first, glue along the fibers following Id
R, and on the second, glue along the fibers following -Id
R.
With that, define now a projection map pr:E-->B that sends [((x,\alpha),y)] to x. This is obviously independent of the class so it is well defined. Now E is a fiber bundle because it is trivializable over the U_\alpha's by the map \Phi_{\alpha}:pr^{-1}(U_{\alpha})\rightarrow U_{\alpha}\times F that says "for a class in pr^{-1}(U_{\alpha}), pick the representative that belongs to U_{\alpha}\times F, say ((x,\alpha),y), and send it to (x,y)". Now suppose \beta is another index. How does \Phi_{\beta}:pr^{-1}(U_{\beta})\rightarrow U_{\beta}\times F acts on the same element [((x,\alpha),y)] of E? Well, it says "pick the representative that belongs to U_{\beta}\times F... well that's ((x,\beta),g_{\alpha\beta}y) by definition of the equivalence relation! So send it to (x,g_{\alpha\beta}y)."
So you see, the transition function associated with the trivialisations \Phi_{\alpha} and \Phi_{\beta} is g_{\alpha\beta}, in the sense that \Phi_{\beta}\circ\Phi_{\alpha}^{-1}(x,y)=(x,g_{\alpha\beta}y).