The fold tensor product of is denoted by . Since
it is a free -module, as well, we may apply all results of
former sections to a situation where is substituted by ,
by
and by
. There are
natural isomorphisms between and
and between
and
. We will omit
them in our notation and consider them as identity maps. Set
.
Suppose we are given a family of -algebras such that . According to lemma 2.1 there is an associated family of coideals in .
By the above identification we consider
as the tensor algebra on the -module .
There is a unique coalgebra structure on this tensor algebra, extending
the one from and turning
into a bialgebra.
Furthermore the
are subcoalgebras dual to the algebras
, i.e. the coalgebra structure on
is the one considered
above.
Epimorphic images of this bialgebra are called matric bialgebras
(cf. [Ta]).
Let us investigate under what circumstances the coideal
PROOF: First we show that is a homogenous ideal. To this claim take
and
. We have to show
and
. The choice of the element
can be reduced to a generator
of the -module
with
and
.
Letting
and
, where
is the preimage of
under
one obtains
For the second part denote by the homogenous ideal in
generated by . Since is a homogenous ideal
containing we get . For the reverse inclusion we
show
by induction on . Clearly
and are contained in . Now suppose .
Letting
one obtains
. By induction hypothesis we see
. Therefore
According to the proposition we may assign a
graded matric bialgebra to each subset
by
An application where must consist of two elements will be given in
the next section. Here the are images of the Brauer
centralizer algebras under Brauer's representations corresponding
to the symplectic groups. The bialgebra will turn out to be
the coordinate ring of a certain symplectic monoid.
It is a remarkable fact, that the second operator is only needed
in the classical situation, whereas in the quantum case it lies in the
algebraic span of the quantum Yang-Baxter operator (see [Oe],
Bemerkung 2.5.1, 2.5.4). Thus, the ordinary FRT-construction behaves
singularly (in a certain sense) when specializing the deformation parameter
to 1, i.e. in the classical limit.
We close this section giving a more convenient description of . We denote by the set of maps from from to and call the elements multi-indices writing , where for . The residue classes of the multiplicative generators of where will be denoted by . For pairs of multi-indices we introduce the abbreviation
Using the notation introduced in (1) we obtain a presentation of by generators and relations given as follows
The verification of this formula follows from the second statement of proposition 5.1 together with (2).