superpotentials
It’s been a while, so let’s include a recap : a (transitive) permutation representation of the modular group
is determined by the conjugacy class of a cofinite subgroup
, or equivalently, to a dessin d’enfant. We have introduced a quiver (aka an oriented graph) which comes from a triangulation of the compactification of
where
is the hyperbolic upper half-plane. This quiver is independent of the chosen embedding of the dessin in the Dedeking tessellation. (For more on these terms and constructions, please consult the series
Modular subgroups and
Dessins d’enfants).
Why are quivers useful? To start, any quiver
defines a noncommutative algebra, the path algebra
, which has as a
-basis all oriented paths in the quiver and multiplication is induced by concatenation of paths (when possible, or zero otherwise). Usually, it is quite hard to make actual computations in noncommutative algebras, but in the case of path algebras you can just see what happens.
Moreover, we can also see the finite dimensional representations of this algebra
. Up to isomorphism they are all of the following form : at each vertex
of the quiver one places a finite dimensional vectorspace
and any arrow in the quiver
determines a linear map between these vertex spaces, that is, to
corresponds a matrix in
. These matrices determine how the paths of length one act on the representation, longer paths act via multiplcation of matrices along the oriented path.
A necklace in the quiver is a closed oriented path in the quiver up to cyclic permutation of the arrows making up the cycle. That is, we are free to choose the start (and end) point of the cycle. For example, in the one-cycle quiver
![\xymatrix{\vtx{} \ar[rr]^a & & \vtx{} \ar[ld]^b \\ & \vtx{} \ar[lu]^c &} \xymatrix{\vtx{} \ar[rr]^a & & \vtx{} \ar[ld]^b \\ & \vtx{} \ar[lu]^c &}](/latexrender/pictures/35440701b59e55eed3f49ecc53aa8325.gif)
the basic necklace can be represented as
or
or
. How does a necklace act on a representation? Well, the matrix-multiplication of the matrices corresponding to the arrows gives a square matrix in each of the vertices in the cycle. Though the dimensions of this matrix may vary from vertex to vertex, what does not change (and hence is a property of the necklace rather than of the particular choice of cycle) is the trace of this matrix. That is, necklaces give complex-valued functions on representations of
and by a result of
Artin and Procesi there are enough of them to distinguish isoclasses of (semi)simple representations! That is, linear combinations a necklaces (aka super-potentials) can be viewed, after taking traces, as complex-valued functions on all representations (similar to character-functions).
In physics, one views these functions as potentials and it then interested in the points (representations) where this function is extremal (minimal) : the vacua. Clearly, this does not make much sense in the complex-case but is relevant when we look at the real-case (where we look at skew-Hermitian matrices rather than all matrices). A motivating example (the Yang-Mills potential) is given in Example 2.3.2 of Victor Ginzburg’s paper Calabi-Yau algebras.
Let
be a super-potential (again, a linear combination of necklaces) then our commutative intuition tells us that extrema correspond to zeroes of all partial differentials
where
runs over all coordinates (in our case, the arrows of the quiver). One can make sense of differentials of necklaces (and super-potentials) as follows : the partial differential with respect to an arrow
occurring in a term of
is defined to be the path in the quiver one obtains by removing all 1-occurrences of
in the necklaces (defining
) and rearranging terms to get a maximal broken necklace (using the cyclic property of necklaces). An example, for the cyclic quiver above let us take as super-potential
(2 cyclic turns), then for example

(the first term corresponds to the first occurrence of
, the second to the second). Okay, but then the vacua-representations will be the representations of the quotient-algebra (which I like to call the vacualgebra)

which in ‘physical relevant settings’ (whatever that means…) turn out to be Calabi-Yau algebras.
But, let us return to the case of subgroups of the modular group and their quivers. Do we have a natural super-potential in this case? Well yes, the quiver encoded a triangulation of the compactification of
and if we choose an orientation it turns out that all ‘black’ triangles (with respect to the Dedekind tessellation) have their arrow-sides defining a necklace, whereas for the ‘white’ triangles the reverse orientation makes the arrow-sides into a necklace. Hence, it makes sense to look at the cubic superpotential
being the sum over all triangle-sides-necklaces with a +1-coefficient for the black triangles and a -1-coefficient for the white ones. Let’s consider an index three example from a previous post
![\xymatrix{& & \rho \ar[lld]_d \ar[ld]^f \ar[rd]^e & \\
i \ar[rrd]_a & i+1 \ar[rd]^b & & \omega \ar[ld]^c \\
& & 0 \ar[uu]^h \ar@/^/[uu]^g \ar@/_/[uu]_i &} \xymatrix{& & \rho \ar[lld]_d \ar[ld]^f \ar[rd]^e & \\
i \ar[rrd]_a & i+1 \ar[rd]^b & & \omega \ar[ld]^c \\
& & 0 \ar[uu]^h \ar@/^/[uu]^g \ar@/_/[uu]_i &}](/latexrender/pictures/aab36d16da83218af03225c806a3d999.gif)
In this case the super-potential coming from the triangulation is

and therefore we have a noncommutative algebra
associated to this index 3 subgroup. Contrary to what I believed at the start of this series, the algebras one obtains in this way from dessins d’enfants are far from being Calabi-Yau (in whatever definition). For example, using a GAP-program written by
Raf Bocklandt Ive checked that the growth rate of the above algebra is similar to that of
, so in this case
can be viewed as a noncommutative curve (with singularities).
However, this is not the case for all such algebras. For example, the vacualgebra associated to the second index three subgroup (whose fundamental domain and quiver were depicted at the end of
this post) has growth rate similar to that of
…
I have an outlandish conjecture about the growth-behavior of all algebras
coming from dessins d’enfants : the algebra sees what the monodromy representation of the dessin sees of the modular group (or of the third braid group).
I can make this more precise, but perhaps it is wiser to calculate one or two further examples…
(limit over all finite index normal subgroups
) gives an embedding of the sets of (continuous) simple finite dimensional representations
we would like the above embedding to be dense in some kind of noncommutative analogon of the
.
as in
be the vectorspace with basis the conjugacy classes of elements of
(that is, the space of class functions). As explained
separate finite dimensional (semi)simple representations of 
is dense. For, suppose it would be contained in a proper closed subset then there would be a class-function vanishing on all simples of
so, in particular, there should be a bound on the number of simples of finite quotients
which clearly is not the case (just look at the quotients
).
.
which is an linear functional on the noncommutative functions
and defined via
for all 

into the linear dual of
. This is a consequence of the celebrated Artin-Procesi theorem.
of all n-dimensional representations of A on which the group
acts via basechange, the orbits of which are exactly the isomorphism classes of representations. He went on to use the Hilbert criterium in invariant theory to prove that the closed orbits for this action are exactly the isomorphism classes of semi-simple -dimensional representations. Invariant theory tells us that there are enough invariant polynomials to separate closed orbits, so we would be done if the caracters would generate the ring of invariant polynmials, a statement first conjectured in this paper.
matrices” in which he reformulated the fundamental theorems on
). Using the properties of the Reynolds operator in invariant theory it then follows that the same applies to the
-algebra A is generated by the elements
then we define a necklace to be an equivalence class of words in the
, where two words are equivalent iff they are the same upto cyclic permutation of letters. For example
and
determine the same necklace. Remark that traces of different words corresponding to the same necklace have the same value and that the noncommutative functions
are spanned by necklaces.
as elements of
This morning,
for some invertible n by n matrix g) ??? So,
does there exist a sort of Jordan normal form for couples of n by n
matrices which are sufficiently general? That is, are there a set of
invariants for such couples which determine it is freely upto
simultaneous conjugation?
For couples of 2 by 2 matrices,
The case of couples of 3 by 3 matrices was finally
settled in 1979 by
Fortunately, early 1990, together with
