Geometric Representation Theory (Lecture 22)
Posted by John Baez
This time in the Geometric Representation Theory Seminar, Jim introduces a new example: the Hall algebra of a quiver.
I talked about Hall algebras back in “week230”; now we’re going to groupoidify them. Hall algebras are exciting because they’re a slick way to get a quantum group from an type Dynkin diagram — or at least the top half of a quantum group.
Let me recall some stuff from “week230”, where I explained the the Hall algebra of an abelian category .
As a set, this consists of formal linear combinations of isomorphism classes of objects of . No extra relations! It’s an abelian group with the obvious addition. But the cool part is, with a little luck, we can make it into a ring by letting the product be the sum of all isomorphism classes of objects weighted by the number of isomorphism classes of short exact sequences
This only works if the number is always finite.
The fun starts when we take the Hall algebra of , where is a quiver. We could look at representations in vector spaces over any field, but let’s use a finite field - necessarily a field with elements, where is a prime power.
Then, Ringel proved an amazing theorem about the Hall algebra when comes from a Dynkin diagram of type , , or :
- C. M. Ringel, Hall algebras and quantum groups, Invent. Math. 101 (1990), 583-592.
He showed this Hall algebra is a quantum group! More precisely, it’s isomorphic to the -deformed universal enveloping algebra of a maximal nilpotent subalgebra of the Lie algebra associated to the given Dynkin diagram.
That’s a mouthful, but it’s cool. For example, the Lie algebra associated to is , and the maximal nilpotent subalgebra consists of strictly upper triangular matrices. We’re -deforming the universal enveloping algebra of this. One cool thing here is that the "q" of q-deformation, familiar in quantum group theory, gets interpreted here as a prime power - something we’ve already seen in "week185" and subsequent weeks.
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Lecture 22 (Jan. 10) - James Dolan on groupoidifying the Hall algebra of an abelian category. Any abelian category A gives a “trispan” of groupoids: namely, three functors from the groupoid
of short exact sequences in A to the underlying groupoid of A,
say A0. These three functors send any exact sequence
to the subobject , the quotient object and the ‘total’ object , respectively.
Degroupoidifying we get a vector space — this consists of formal linear combinations of isomorphism classes of objects of . Ignoring possible divergences, degroupoidifying the trispan then gives a product
A magical fact: this product is associative, making into an associative algebra called the Hall algebra of . So, we have groupoidified the Hall algebra.
The classic example arises when is the category of representations of a quiver on vector spaces over the field with elements, . The simplest example: the quiver , which looks like this:
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- Lecture notes by Alex Hoffnung
- Lecture notes by Apoorva Khare
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Re: Geometric Representation Theory (Lecture 22)
There’s now a downloadable version of the video for this seminar! Check it out and see if it works for you.