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.