I heard that in complex hyperbolic space setting for example CH2, there is some deformation of lattice nontrivial. What confused me is it seems contradicting Mostow Rigidity. Could someone explain this?
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2$\begingroup$ Please state precisely what you heard. Most likely, it concerned infinite covolume isometry groups. Even in that case there is a lot of rigidity (due to Goldman-Millson and hence generalized in various ways, see e.g. arxiv.org/abs/0903.3706). $\endgroup$– Igor BelegradekCommented Jul 25, 2014 at 15:15
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$\begingroup$ actually the example i see is the deformation of scokotty group and the ICM talk of Schwatz. Does Strong rigidity rules out all the possibility of nontrivial deformation of lattice(Even in rank one)except PSL(2,R)? $\endgroup$– user42804Commented Jul 26, 2014 at 6:56
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1$\begingroup$ Your examples are of infinite covolume. Yes, Mostow rigidity (or even the Weil rigidity mentioned by Andy Sanders) rules out deformations of a lattice in the associated Lie group, but the lattice could a priori be deformed in a bigger Lie group. This is discussed in the paper I linked aboved. $\endgroup$– Igor BelegradekCommented Jul 26, 2014 at 11:42
1 Answer
It follows from Weil's rigidity theorem http://www.jstor.org/stable/1970212 that given any uniform lattice in $SU(n,1)$ with $n>1,$ it has no local deformations, in fact no non-trivial first order deformations. If $n=1$ then the the symmetric space is the real hyperbolic plane and there is a large family of deformations for surface groups.
Now, if you don't require the lattice condition, then there may or may not be deformations. The case of a surface group is the most well understood (to me at least). It is a theorem of Toledo that a discrete surface group (here surface means closed, oriented and genus at least two) in $SU(2,1)$ which stabilizes a totally geodesic holomorphic hyperbolic plane in $\mathbb{CH}^2$ is locally rigid. But, surfaces groups which stabilize a totally real lagrangian hyperbolic plane in $\mathbb{CH}^2$ admit many deformations, these are so-called complex hyperbolic quasi-Fuchsian groups and their deformations are still far from well understood. Maybe Misha Kapovich (who posts here and is an expert) might add some more interesting comments at some point.