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May 14, 2012 at 2:15 vote accept Earthliŋ
May 14, 2012 at 2:14 comment added Earthliŋ Many thanks for your detailed answer & comments.
May 13, 2012 at 21:37 comment added Misha The product bundle $\tilde{M}\times G$ has obvious flat connection, where horizontal leaves are of the form $\tilde{M}\times g$. This connection is preserved under the action of $\pi$ and, hence, descends to the flat connection on the principal bundle $P_\phi\to M$, $P_\phi=(\tilde{M}\times G)/\pi$. Conversely, every flat principal $G$-bundle $P\to M$ bundle has monodromy representation $\phi$, so that $P\cong P_\phi$ as a flat $G$-bundle. This relation of flat connections and representations is explained in many places, e.g. Steenrod's book on fiber bundles.
May 13, 2012 at 21:31 comment added Misha @ s.barmeier: You do not need to assume that $\phi$ is a discrete embedding. The relation between representations of a group $\pi$ (endowed with discrete topology) to a Lie group $G$ and flat principal $G$-bundles over $M$ (where $M$ is any CW-complex with fundamental group $\pi$) is very general and standard. For instance, if you have a representation $\phi: \pi\to G$, form the associated bundle over $M$ by taking $(\tilde{M}\times G)/\pi \to M$, where $\pi$ acts on the first factor by covering transformations and on the second factor via left multiplication $\phi(\gamma)(g)$...
May 13, 2012 at 4:03 comment added Earthliŋ I'm missing the "very simple" bit. I can't quite see the holonomy group. Is the flatness somehow related to $\pi$ being discrete (and $\phi$ being a discrete embedding)? I'm also stumbling a bit over the notation. What is the base manifold in this case, and what is $A$?
May 13, 2012 at 3:10 history edited Misha CC BY-SA 3.0
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May 13, 2012 at 2:59 comment added Misha For your last question, see the reference in the Addendum.
May 13, 2012 at 2:58 comment added Misha Yes, this functor is equivalent to the functor defined by DGLAs. The origin of this result is very simple: $Hom(\pi, G)$ can be identified with the space of (normalized) flat connections on the base-manifold. Flat connections lead to DGLAs, since a connection can be locally written as $d +A$: The exterior differential $d$ (with values in an appropriate Lie algebra) is responsible for differential in DGLA, while Lie comes from the fact that everything is taking values in a Lie algebra, so you have the Lie bracket, graded comes from natural grading on differential forms.
May 13, 2012 at 2:52 history edited Misha CC BY-SA 3.0
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May 13, 2012 at 0:59 comment added Earthliŋ Oh, and why do we know that singularities can be arbitrarily complicated?
May 13, 2012 at 0:53 comment added Earthliŋ Maybe this should be a new question, but I had a look at the paper of Goldman & Millson. It seems like they end up studying differential graded Lie algebras. How exactly does this tie in with the example you give? I guess $\mathrm{Hom}_\rho(\pi,\underline{G})$ as a functor is somehow equivalent to a deformation functor of the DGLA?
May 13, 2012 at 0:13 history edited Misha CC BY-SA 3.0
relation to Artin local rings
May 12, 2012 at 16:47 history edited Misha CC BY-SA 3.0
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May 12, 2012 at 16:39 history edited Misha CC BY-SA 3.0
added slice discussion
May 12, 2012 at 16:23 comment added Misha See "Addendum."
May 12, 2012 at 14:38 history edited Misha CC BY-SA 3.0
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May 12, 2012 at 13:41 comment added Earthliŋ Great, that is really interesting. Are there any references for these character varieties $\mathrm{Hom}(\Gamma,G)$ and their quotients? I'm not quite following your point near the end. Are you saying that for discrete and faithful representations the right quotient can always be isolated? Or is that a particular feature of Teichmüller theory, which uses particularly nice features of $\mathrm{SL}_2\,\mathbb{R}$? I would be really grateful for a reference for this process of taking slices as well.
May 12, 2012 at 12:59 history answered Misha CC BY-SA 3.0