non-commutative geometry
- Brauer’s forgotten group
- connected component coalgebra
- Galois and the Brauer group
- a noncommutative Grothendieck topology
- noncommutative geometry
- noncommutative geometry 2
- projects in noncommutative geometry
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- more noncommutative manifolds
- the necklace Lie bialgebra
- the one quiver for GL(2,Z)
- representation spaces
- quiver representations
- moduli spaces
- cotangent bundles
- differential forms
- curvatures
- Brauer-Severi varieties
- smooth Brauer-Severis
- hyper-resolutions
- a cosmic Galois group
- double Poisson algebras
- A for aggregates
- B for bricks
- necklaces (again)
- seen this quiver?
- why nag? (2)
- why nag? (3)
- sexing up curves
- the Klein stack
- Alain Connes on everything
- noncommutative topology (1)
- a noncommutative topology 2
- noncommutative topology (3)
- noncommutative topology (4)
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- non-(commutative) geometry
- noncommutative Fourier transform
- noncommutative bookmarks
- noncommutative geometry : a medieval science?
Last time we saw that for $A$ a smooth order with center $R$ the
Brauer-Severi variety $XA$ is a smooth variety and we have a projective
morphism $XA \rightarrow \mathbf{max}~R$ This situation is
very similar to that of a desingularization $~X \rightarrow
\mathbf{max}~R$ of the (possibly singular) variety $~\mathbf{max}~R$.
The top variety $~X$ is a smooth variety and there is a Zariski open
subset of $~\mathbf{max}~R$ where the fibers of this map consist of just
one point, or in more bombastic language a $~\mathbb{P}^0$. The only
difference in the case of the Brauer-Severi fibration is that we have a
Zariski open subset of $~\mathbf{max}~R$ (the Azumaya locus of A) where
the fibers of the fibration are isomorphic to $~\mathbb{P}^{n-1}$. In
this way one might view the Brauer-Severi fibration of a smooth order as
a non-commutative or hyper-desingularization of the central variety.
This might provide a way to attack the old problem of construction
desingularizations of quiver-quotients. If $~Q$ is a quiver and $\alpha$
is an indivisible dimension vector (that is, the component dimensions
are coprime) then it is well known (a result due to
Alastair King)
that for a generic stability structure $\theta$ the moduli space
$~M^{\theta}(Q,\alpha)$ classifying $\theta$-semistable
$\alpha$-dimensional representations will be a smooth variety (as all
$\theta$-semistables are actually $\theta$-stable) and the fibration
$~M^{\theta}(Q,\alpha) \rightarrow \mathbf{iss}{\alpha}~Q$ is a
desingularization of the quotient-variety $~\mathbf{iss}{\alpha}~Q$
classifying isomorphism classes of $\alpha$-dimensional semi-simple
representations. However, if $\alpha$ is not indivisible nobody has
the faintest clue as to how to construct a natural desingularization of
$~\mathbf{iss}{\alpha}~Q$. Still, we have a perfectly reasonable
hyper-desingularization $~X{A(Q,\alpha)} \rightarrow
\mathbf{iss}{\alpha}~Q$ where $~A(Q,\alpha)$ is the corresponding
quiver order, the generic fibers of which are all projective spaces in
case $\alpha$ is the dimension vector of a simple representation of
$~Q$. I conjecture (meaning : I hope) that this Brauer-Severi fibration
contains already a lot of information on a genuine desingularization of
$~\mathbf{iss}{\alpha}~Q$. One obvious test for this seemingly
crazy conjecture is to study the flat locus of the Brauer-Severi
fibration. If it would contain info about desingularizations one would
expect that the fibration can never be flat in a central singularity! In
other words, we would like that the flat locus of the fibration is
contained in the smooth central locus. This is indeed the case and is a
more or less straightforward application of the proof (due to Geert Van
de Weyer) of the Popov-conjecture for quiver-quotients (see for
example his Ph.D. thesis
Nullcones of quiver representations).
However, it is in general not true that the flat-locus and central
smooth locus coincide. Sometimes this is because the Brauer-Severi
scheme is a blow-up of the Brauer-Severi of a nicer order. The following
example was worked out together with
Colin Ingalls : Consider the
order $~A = \begin{bmatrix} C[x,y] & C[x,y] \ (x,y) & C[x,y]
\end{bmatrix}$ which is the quiver order of the quiver setting
$~(Q,\alpha)$
then the Brauer-Severi fibration
$~XA \rightarrow \mathbf{iss}{\alpha}~Q$ is flat everywhere except
over the zero representation where the fiber is $~\mathbb{P}^1 \times
\mathbb{P}^2$. On the other hand, for the order $~B =
\begin{bmatrix} C[x,y] & C[x,y] \ C[x,y] & C[x,y] \end{bmatrix}$
the Brauer-Severi fibration is flat and $~XB \simeq \mathbb{A}^2 \times
\mathbb{P}^1$. It turns out that $~XA$ is a blow-up of $~X_B$ at a
point in the fiber over the zero-representation.
Azumaya, Brauer, Brauer-Severi, moduli, non-commutative, representations
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Posted in geometry
Written on Thu, 30 September 2004 at 4:07 pm
Tags: Azumaya, Brauer, Brauer-Severi, moduli, non-commutative, representations
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