The calculus of bideterminants is needed inside
.
Unless otherwise stated the rules hold in
too. Recall the definition of
from
section 3.
PROOF: Let us first reduce to the case
. Setting
,
,
,
and
We proceed by induction on , the case
being clear.
The case
can be handled immediately with the help of the
above recursion formula. If
we calculate
But by the braid relations we get
yielding the right hand side factorization of . The other formula
is obtained similarly.
PROOF: By assumption,
lies in the kernel of
. Consequently the assertion concerning
follows immediately from
Lemma 9.1 since
.
Using the matrix transposition map
introduced in
section 8, the formula for exchanged multi-indices follows
as well.
Next, we investigate the transition from
to its epimorphic image
.
For this purpose
denote by
the ideal
generated by
in the algebraic span
of the endomorphisms
and
. By equation (1) the realtion
holds in
. By the
braid relations
the relations
and
must hold
in
for all
as well.
The Iwahori-Hecke algebra
of type
is defined
on generators
for
by relations
Therefore,
there is an epimorphism from
to
the quotient
sending the generator
to
(notation as in [DD]).
PROOF: We have to show that
for all
. Let
be such
that
. From the defining equation of the quantum coefficient
of dilation
from section 4 we have
This means
in
for all
. By (5) we have
and therefore,
where
,
and
are the coefficient matrices of
and
.
We extend the notation introduced in
(2). Let
be an endomorphism of
. Set
Similar expressions are used with respect to the capital
notation for bideterminants.
PROOF: Modulo
we have
since the corresponding equations (where is replaced by
)
hold in the Iwahori-Hecke algebra
.
Thus the assertion follows from Lemma 9.3.
Let
denote the ideal in the tensor algebra
generated by the twofold invariant
tensor
and let
be
its
-th homogeneous summand.
PROOF: Since
and
for all
with
by section 4 it follows that
is contained in
. The verification of the opposite inclusion can be reduced to consider
elements of the form
with
for some
. But such an element can be
written as
for some
. Thus the assertion follows.
PROOF: First, note that the second equation follows from the first one by definition
of bideterminants.
By the above lemma we can reduce to the case
where
and
. Thus we get
Next, we give a quantum symplectic version of Laplace duality. The corresponding classical result can be found in [Ma, 2.5.1], for instance.
PROOF: Using the disjoint union
and the fact
,
which holds by length additivity
we calculate
The next result is needed for the transition from
-bideterminants of compositions
to
-bideterminants of
partitions.
PROOF: First, there is a permutation
, such that
is a partition. This
is uniquely determined by
(but
only under the restriction to be of minimal length).
Clearly the parabolic subgroups
and
in
are conjugate to each other. Thus, there
is an element
such that
. Furthermore, it is known
from the theory of parabolic subgroups that in the left coset
and in the right coset
there are unique representatives
(resp.
)
of minimal length. Since we have
for all
and
for all
, we have
.
By the definition of bideterminants
(
),
the relations (5)
holding inside
and the calculus for the symbol
given in
(3) we obtain
Since
this results in
Next, we introduce a calculus for our bideterminants bringing
our special order on
into the picture. First,
some new notation has to be explained. The sum of two
multi-indices
and
is
defined by juxtaposition, that is
Note that the map
occurring in
Theorem 8.3
is additive in the sense
. This implies
with respect to the lexicographic order on
.
To a multi-index
we consider the following
-spans
in
:
Furthermore, we set
and denote the simple transpositions by
, as before.
The following lemma is the key concerning calculations with bideterminants.
Again we set
.
PROOF: The congruence relation for
follows from the one for
because
by (1).
Therefore, it is enough to prove the first assertion.
First, consider the case
. If
,
the asserted congruence relation is also an equation, as can be seen directly
from the definition of
. Turning to the case
, we split
into three summands
To
we set
and calculate
Since
we obtain the equation
But
and
for all by (11), yielding the asserted congruence
modulo
. If
the interesting case is
. Here the assertion immediately follows from
the calculation
because
for all
.
PROOF: Note that
is the
coefficient of
in the
expression
.
By definition of bideterminants and the conventions (10)
about
, the result follows immediately from the lemma.
PROOF: We use induction on the length of .
If this is zero there is nothing to prove.
If not, we write
where
and
.
By the induction hypothesis we have
Here we have set
,
where the product runs over all pairs
such that
.
PROOF: We use induction on , the case
being trivial.
For
we embed
as the parabolic subgroup of
generated by
, which fix
.
If
there is nothing to prove by the induction
hypothesis. Otherwise, we write
where
and
for an appropriate
, thus
. By the induction hypothesis, Lemma 9.9
and Remark 9.10 we calculate
PROOF: As for the proof of Corollary 9.11, this follows
easily from the preceding lemma, Lemma
and the definition of bideterminants.