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2023-07-25
- problem with torsion in .
Torsion
So, what's the difference between ? is the father of all, and each take out some abelian part out of it. totally killed the central subgroup, by quotienting out it, whereas tries to take a slice, that intersects minimally with it.
Then, the composition is a finite cover. This has many immediate consequences
- The cocharacter lattice is injective. This is because is only left exact, not right exact, hence loses surjectivity, we are led to . If the target is a discrete group , then .
- The character lattice, , seems to be injective. Is it because is exact? Here, if is a finite abelian group, then is just the 'Pontryagin dual'.
So far so good. Now because of is surjective, hence, we have any representation of goes to rep of , no loss of information.
How about the functions on and ? If we ignore -invariance, we have more functions on . Basically, the deck transformation is transparent to action. This also matches with . I would also say, , which is also the center of . They are canonically the same. (no funny dual involved). Indeed, this is also the deck transformation of . the thing you quotient by become the fundamental group of the base.
So, we should have , just because has more representations. How does the folding affect the quotient? Well, say for coordinate and coordinate , action changes to , hence to . The thing that I don't quite understand is: when we fold to , there are two fixed points , but these should get quotient out by . But then, new fixed points pop up.
What's the class function ring for ? They are function on , that is invariant under rescaling and conjugation. So, we need to divide out by determinant, which is a homogenous degree guy. We basically only know about eigenvalues, say .
OK, fine. Now, how about ? What does know? T knows and . So you imagine, we should get , but indeed we get that. So, what is the problem?
http://math.stanford.edu/~conrad/210CPage/handouts/repring.pdf
What are you saying? Here, is a connected compact Lie group, maximal torus.
Well, from the notion of a Lie algebra alone, we should get the notion of root , coroot , then the weight lattice (integral dual to the ) and coweight lattice, integral dual to . All that come for free, if you give me a Lie algebra. Now, if you give me a group form, then I have a torus, then I can do character and cocharacters. We should have , and .
Now, if is simply connected, then is big (others are a quotient of it), so (yes, lots of representations), and (is small) is . If has trivial center, then it is the other way around, , the adjoint type.
First thing I learned, the derived subgroup (generated by commutator), is not necessary of adjoint-type. Why we want it? To kill as much torus as possible? Does this guy have finite ? Should be. Is it semi-simple? OK, there are some torus part, and there are some semi-simple part,then we marry them together.
Ex 1: , it is
Ex 2: , it is
Well, why do we need to take the universal cover? Why cannot we just take the derived subgroup, then times the torus, and quotient by something? Well, can only be a torus? That makes it even more suspicious!
OK, so what? You have some finite group acting on the coordinate ring of the torus. You take invariant.
So, what is this? Well, I think the best way is not to quotient, but remember the action.
So, what is the answer, for ? The answer for K-Coulomb? What is the naive answer? The base should be still . Well, we have . That is , with acting with different powers (indicated in the lower indices).
BFM says it is , fibered to the base .
What is . So, if and , you have the quotient torus and subtorus . Then, the root is like on , and on , it is like . So, we have Look, what happens when , and ? These are also fixed points of , but there is no blow-up to resolve it.
Do we have that problem in general?