Let be a holomorphic line bundle over a complex manifold . The total space of this bundle is a complex manifold in its own right, and it contains the smooth hypersurface , which is embedded as the set of zero vectors. Let denote the complement.
Let be a complex Lie group. In this post we will study principal -bundles that are equipped with connections which are flat and have logarithmic singularities along . Denote the category of these connections . Given any connection , we can restrict it to , where it defines a non-singular flat connection. By the Riemann-Hilbert correspondence, is equivalent to a homomorphism
In fact, we get a ‘restriction functor’
Question : Does every -representation of come from an object of ?
When the group , Deligne’s construction answers this question in the affirmative. In a previous blog post, I explained this construction, as well as some of the required background on flat logarithmic connections. A key tool in this construction is the fact, explained in another blog post, that a set-theoretic logarithm determines canonical matrix logarithms. This fact about is not shared by other groups, and hence Deligne’s construction does not extend. The purpose of this post is to give a counterexample to the Question when .
In order to construct the counterexample, I will use a description of the category that I provided in my paper. This applies in the case that is complex and reductive, but for this post, I will stick to the case of .
A few preliminary concepts to start. First, the fundamental group of the complement . It is a -bundle over , and hence the fundamental groups of , , and are related to each other through an exact sequence:
This sequence is a portion of a long exact sequence relating all the homotopy groups. Such a sequence exists for any fibration. In this sequence, , and the generator corresponds to a loop that goes once around the fiber. It maps to a loop which is a central element of the group. In the picture above, I drew it as a purple loop.
Next, the residue of a connection. Let be a connection. In a neighbourhood of a point of , we can trivialize the bundle and express the connection as follows:
Here are local coordinates on , with the coordinate on the fibre which vanishes along , and and are holomorphic functions valued in , the matrices with zero trace. The residue of is the element
The way I’ve stated it doesn’t quite make sense, since apparently depends on , and on the choice of a trivialization of . There is a more invariant definition of the residue which deals with all these issues, but all you need to know for now is that is well-defined up to conjugation. The residue is an invariant of the connection, and it makes sense to fix it (i.e. its conjugacy class). So let denote the full subcategory of connections whose residue is conjugate to .
Now consider an element . By conjugating it, we can put it into Jordan normal form:
where and are real. This leads to a well-defined decomposition , where
We will associate a bunch of subgroups of to the element . First, we define the parabolic subgroup associated to . If , then . If , then it has a unique positive eigenvalue , and a negative eigenvalue . The corresponding eigenspaces give a decomposition of :
The parabolic is defined to be the subgroup of elements which preserve the positive eigenline: . Using the eigenspace decomposition as a basis of , the parabolic consists of elements of the following form
In this basis, the diagonal matrices define the centralizer of : . The elements which restrict to the identity on the positive line define the unipotent radical of :
You should check that is a normal subgroup of , that it has trivial intersection with , and that any element of can be written as a product of elements from these two subgroups. Therefore, the parabolic is a semidirect product of the two groups:
and there is a canonical projection map . By the way, if then , and is trivial.
Okay, with all of this set-up out of the way, I can define a fairly simple category. First, given the element , the exponential . Let denote its conjugacy class. Now define the set
Recall that is the central element corresponding to the loop in the fibre of . The parabolic group acts on by conjugation. Hence we can define the following action groupoid
The objects of this category are the elements , and the morphisms are the pairs . More precisely, is a morphism going between and .
Now I can finally state the classification theorem, which is adapted from Theorem 5.2 of my paper.
Theorem. Let . There is an equivalence of categories
Let’s look at a few simple examples. First, if , then , , and . In this case, consists of homomorphisms satisfying . These homomorphisms factor through . In other words, these are precisely the representations that are pulled back from homomorphisms . Hence, in this case we get
For the second isomorphism, we’ve used the fact that retracts onto and so has isomorphic fundamental group. This makes sense: looking back at the local expression for a connection, we see that if the residue vanishes, then the connection is actually smooth on all of .
Next, let’s take with . Then
And since is commutative, the conjugacy class consists of a single element
The set therefore consists of homomorphisms such that
Okay, back to the main question. Given our new description of the category of representations, our restriction functor is simply given by forgetting the parabolic . More precisely, an object is sent to , viewed now as a homormophism . So to provide a counterexample to the question, we need to give a representation of , and then somehow argue that it could not have come from any of the categories . To simplify things, let’s assume that the line bundle is trivial , so that , and . And to make our life even more simple, let’s postpone choosing the representation of , and focus first on the monodromy If this is going to work, must centralize the representation of , and this is guaranteed if lies in the centre of . This centre is given by
Choosing won’t work, because then we can always solve the problem with . So lets take . No matter what turns out to be, we must have and . This implies that is diagonalizable, and can be taken to be of the form
with satisfying . Hence . In particular, must be non-vanishing and real, and we may assume that it is positive. The group is therefore the group of elements preserving the line . Hence we obtain the following result.
Theorem. Let be a homomorphism such that . If is the monodromy of a flat connection on with logarithmic singularities along , then there exists a line which is preserved by , for all . In particular, is not an irreducible representation of .
This theorem provides a way of constructing a counterexample. Namely, let be an irreducible representation, and define
Then the theorem says that does not extend to a logarithmic connection on .
It is easy to produce such irreducible representations. Here’s a fun example. Let be the braid group on three strands. It has the following presentation:
This group has a representation into given as follows:
To see this, just check that the relation is satisfied. It’s also easy to see that this representation does not fix any line . Indeed, the only line fixed by is the span of , and the only line fixed by is the span of .
I know of at least two ways of realizing as the fundamental group of a complex manifold. First, let’s think of elements of as braids on three strands. Namely, we have three bits of string, and we twist them up as follows.
Viewing this as a movie where time goes upwards, this is the motion of three distinct points in the plane. In other words, this is a path in the space of triples of distinct points in the complex plane . Thinking of these points as the components of a vector in , we can think of this as a path in the following space
A loop in this space corresponds to those braids where the points end up where they started. These are the pure braids, and hence is the pure braid group. In order to get the full braid group, we need all permutations etc. to count as the same, so that any braid gives a loop. So we simply take the quotient by the permutation action
Then .
The second way of realizing as a fundamental group comes from an alternate presentation:
This is the presentation of as a knot group: it is the fundamental group of the complement of the trefoil knot in the three-dimensional sphere. It takes a bit of thinking to see this, but this knot complement is homotopic to the complement of the complex curve in . Hence,
In fact, there is yet another way of realizing as a fundamental group. This paper proves that every finitely presented group can be realized as the fundamental group of a compact complex 3-manifold.