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Vector bundles and Hermitian
operators
Alexander A. Klyachko
Abstract. We'll deal with three apparently disjoint problems:
-
1.
-
The spectrum of a sum of Hermitian operators,
-
2.
-
Components of tensor product of irreducible representations of the group
,
-
3.
-
Structure of the moduli space of stable bundles on the projective plane
.
1. Hermitian operators
We begin with the first subject. Let
be a Hermitian operator in a unitary space E of finite dimension
n and let
be its spectrum. The problem is to find all restrictions on spectra
and
.
First of all we have trace identity
and a number of classical inequalities, all of the form
|
 |
(IJK) |
for some triple of subsets
of the same cardinality.
Let us fix a decomposition n=p+q. We have a bijection
between subsets
of cardinality p=|I| and Young diagrams
in a rectangular box of dimension p (North) by q (East) given
as follows. Let
be a polygonal line with unit edges that runs from the South-West corner
of the box to the East-North corner with the i-th edge running to
the North for
and to the East otherwise. The line
cuts out from the box a Young diagram
situated in its North-West angle. The diagram
in the usual way corresponds to a Schubert cycle sI in
a Chow ring of the Grassmannian.
Theorem 1.1. Consider a triple of subsets
such that the Schubert cycle sK is a component of
.
Then
-
i)
-
The inequality (IJK) holds.
-
ii)
-
In union with the trace identity, this inequalities form a complete
set of restrictions on spectra of A,B and A+B.
2. Tensor Products
Let us consider an integer spectrum
and associate with it the following dominant weight of general linear group
The weight
in the usual way corresponds to an irreducible representation
of the group
with highest weight
.
We are iterested in the problem: which irreducible representations
are components of tensor product
?
The result is that the inequalities (IJK) of Theorem 1.1 answer this question
too. More precisely,
Theorem 2.1. The irreducible representation
is a component of tensor product
for some positive N if and only if
and
are spectra of Hermitian operators A,B and C=A+B.
3. Vector bundles
It will be explained in the lecture that both of the previouse theorems
follows from existence of Hermite-Einstein metric on stable toric vector
bundles on
.
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Richard Porter
9/8/1998