ccdantas said:
I've tried to give a general sketchy introduction to Witten's paper in http://math.ucr.edu/home/baez/week254.html" - you might look at that.
Further, what is "holomorphic" factorization? (A pointer to the basic literature on this will suffice).
I don't really understand that term. It should be defined in http://arxiv.org/abs/hep-th/9205072" --- this paper speaks of "meromorphic conformal field theories" instead of "conformal field theories with holomorphic factorization", but they must be the same thing. However, I'm having a bit of trouble finding the precise definition! I just know a bunch of properties of these theories.
First, the central charge c is an integer multiple of 24.
Second, as a consequence, the partition function is really a well-defined number, not just defined up to (24/c)th root of unity. In other words, it's "modular invariant".
These two are very important in Witten's paper.
Third, as another consequence, the http://en.wikipedia.org/wiki/Schwinger_function" --- that is, holomorphic except for poles. This is not so important in Witten's paper, though.
Is it the only possible constraint?
Witten gives an argument that 3d quantum gravity has as its AdS/CFT dual a conformal field theory with c = 24k for some integer k = 1,2,3,... The main
nice thing is that - modulo a certain conjecture - Schellekens classified these conformal field theories for k = 1.
He argues that the (naive) partition function Z_0(q) differs from the "exact" Z(q) by terms of order O(q). Would this be correct for any k?
Yes, he argues this is true for any k. Then, around equation (3.13), he shows that this property, together with modular invariance of the exact partition function, completely determines the exact partition function! It's a certain explicit polynomial in the J function.
He finds that for k=1 the monster group is interpreted as the symmetry of 2+1-dimensional black holes. How sensitive is this result with respect to the value of k, and to respect to the other assuptions used in the derivation?
For k=1 he goes through Schelleken's list of 71 conformal field theories with c = 24 and picks the one that has the Monster group as its symmetries. He gives an argument for why this one is the right one, but it's not airtight.
He doesn't actually find the relevant conformal field theories with c = 24k for
higher values of k. He just figures out their supposed partition functions. Since the coefficients of their partition functions are - just as in the k = 1 case - dimensions of representations of the Monster group, it seems awfully plausible that these theories (if they really exist!) have the Monster group as symmetries.
However, this is something one would want to check. Nobody seems to know a c = 48 theory with Monster group symmetries, for example.
I will copy your questions and my answers to the http://golem.ph.utexas.edu/category/2007/07/this_weeks_finds_in_mathematic_15.html" , and hope some experts on conformal field theory (like
Urs Schreiber and Jacques Distler) can help us out.