The Tenfold Way (Part 4)
Posted by John Baez
Back in 2005, Todd Trimble came out with a short paper on the super Brauer group and super division algebras, which I’d like to TeXify and reprint here.
In it, he gives extremely efficient proofs of several facts I alluded to last time. Namely:
• There are exactly 10 real division superalgebras.
• 8 of them have center , and these are Morita equivalent to the real Clifford algebras .
• 2 of them have center , and these are Morita equivalent to the complex Clifford algebras and .
• The real Clifford algebras obey
where means they’re Morita equivalent as superalgebras.
It easily follows from his calculations that also:
• The complex Clifford algebras obey
These facts lie at the heart of the ten-fold way. So, let’s see why they’re true!
Before we start, two comments are in order. First, Todd uses Deligne’s term ‘super Brauer group’ where I decided to use ‘Brauer–Wall group’. Second, and more importantly, there’s something about Morita equivalence everyone should know.
In my last post I said that two algebras are Morita equivalent if they have equivalent categories of representations. Todd uses another definition which I actually like much better. It’s equivalent, it takes longer to explain, but it reveals more about what’s really going on. For any field , there is a bicategory with
• algebras over as objects,
• - bimodules as 1-morphisms from the algebra to the algebra , and
• bimodule homomorphisms as 2-morphisms.
Two algebras and over are Morita equivalent if they are equivalent in this bicategory; that is, if there’s a - bimodule and a - bimodule such that
as an - bimodule and
as a - bimodule. The same kind of definition works for Morita equivalence of superalgebras, and Todd uses that here.
So, with no further ado, here is Todd’s note.
The super Brauer group and division superalgebras
The super Brauer group
Let be the symmetric monoidal category of finite-dimensional super vector spaces over . By super algebra I mean a monoid in this category. There’s a bicategory whose objects are super algebras , whose 1-morphisms are left - right -modules in , and whose 2-morphisms are homomorphisms between modules. This is a symmetric monoidal bicategory under the usual tensor product on .
and are Morita equivalent if they are equivalent objects in this bicategory. Equivalence classes form an abelian monoid whose multiplication is given by the monoidal product. The super Brauer group of is the subgroup of invertible elements of this monoid.
If is inverse to [A] in this monoid, then in particular can be considered left biadjoint to . On the other hand, in the bicategory above we always have a biadjunction
essentially because left -modules are the same as right -modules, where denotes the super algebra opposite to . Since right biadjoints are unique up to equivalence, we see that if an inverse to exists, it must be .
This can be sharpened: an inverse to exists iff the unit and counit
are equivalences in the bicategory. Actually, one is an equivalence iff the other is, because both of these canonical 1-morphisms are given by the same -bimodule, namely the one given by acting on both sides of the underlying superspace of (call it ) by multiplication. Either is an equivalence if the bimodule structure map
which is a map of superalgebras, is an isomorphism.
As an example, let be the Clifford algebra generated by the 1-dimensional space with the usual quadratic form , and -graded in the usual way. Thus, the homogeneous parts of are 1-dimensional and there is an odd generator satisfying . The opposite is similar except that there is an odd generator satisfying . Under the map
where we write as a sum of even and odd parts , this map has a matrix representation
which makes it clear that this map is surjective and thus an isomorphism. Hence is invertible.
One manifestation of Bott periodicity is that has order 8. We will soon see a very easy proof of this fact. A theorem of C. T. C. Wall is that in fact generates the super Brauer group; I believe this can be shown by classifying super division algebras, as discussed below.
Bott periodicity
That has order 8 is an easy calculation. Let denote the -fold tensor power of . for instance has two supercommuting odd elements satisfying ; it follows that satisfies , and we get the usual quaternions, graded so that the even part is the span and the odd part is .
has three supercommuting odd elements all of which are square roots of . It follows that is an odd central involution (here ‘central’ is taken in the ungraded sense), and also that , , satisfy the Hamiltonian equations
so we have . Note this is the same as
where the here is the quaternions viewed as a super algebra concentrated in degree 0 (i.e. is purely bosonic).
Then we see immediately that is equivalent to purely bosonic (since the cancels in the super Brauer group).
At this point we are done: we know that conjugation on (purely bosonic) gives an isomorphism
hence , i.e. has order 2! Hence has order 8.
The super Brauer clock
All this generalizes to arbitrary Clifford algebras: if a real quadratic vector space has signature , then the superalgebra is isomorphic to , where denotes the -fold tensor product of . By the above calculation we see tha is equivalent to where is taken modulo 8.
For the record, then, here are the hours of the super Brauer clock, where denotes an odd element, and denotes Morita equivalence:
All the superalgebras on the right are in fact division superalgebras, i.e. superalgebras in which every nonzero homogeneous element is invertible.
To prove Wall’s result that generates the super Brauer group, we need a lemma: any element in the super Brauer group is the class of a central division superalgebra: that is, one with as its center.
Then, if we classify the division superalgebras over and show the central ones are Morita equivalent to , we’ll be done.
Classifying real division superalgebras
I’ll take as known that the only associative division algebras over are — the even part of an associative division superalgebra must be one of these cases. We can express the associativity of a superalgebra (with even part ) by saying that the odd part is an -bimodule equipped with a -bimodule map pairing
such that:
If the superalgebra is a division superalgebra which is not wholly concentrated in even degree, then multiplication by a nonzero odd element induces an isomorphism
and so is 1-dimensional over A; choose a basis element for .
The key observation is that for any , there exists a unique such that
and that the -bimodule structure forces . Hence we have an automorphism (fixing the real field)
and we can easily enumerate (up to isomorphism) the possibilities for associative division superalgebras over :
1. . Here we can adjust so that is either or . The corresponding division superalgebras occur at 1 o’clock and 7 o’clock on the super Brauer clock.
2. . There are two -automorphisms . In the case where the automorphism is conjugation, condition for super associativity gives so that must be real. Again can be adjusted so that equals or . These possibilities occur at 2 o’clock and 6 o’clock on the super Brauer clock.
For the identity automorphism, we can adjust so that is 1. This gives the super algebra (where commutes with elements in ). This does not occur on the super Brauer clock over . However, it does generate the super Brauer group over (which is of order two).
3. . Here -automorphisms are given by for . In other words
whence commutes with all elements of (i.e. we can assume wlog that the automorphism is the identity). The properties of the pairing guarantee that for all , so is real and again we can adjust so that equals or . These cases occur at 3 o’clock and 5 o’clock on the super Brauer clock.
This appears to be a complete (even if a bit pedestrian) analysis.
Re: The Ten-Fold Way (Part 4)
While Todd humbly calls his analysis ‘pedestrian’, I am a bit slow at elementary algebraic tricks, so let me expand this a bit more:
He’s starting with the known fact that all automorphisms of are inner and the fact that where is the result of applying an automorphism to , obtaining
then multiplying both sides to get
But this means we can replace by and get a new odd element with
reducing to the case where the automorphism is trivial.