Representations of twisted Yangians associated with skew Young diagrams

Abstract
Let $G_M$ be either the orthogonal group $O_M$ or the
symplectic group $Sp_M$ over the complex field; in the latter case
the non-negative integer $M$ has to be even. Classically, the
irreducible polynomial representations of the group $G_M$ are
labeled by partitions $\mu=(\mu_{1},\mu_{2},\,\ldots)$
such that $\mu^{\prime}_1+\mu^{\prime}_2\le M$ in the case $G_M=O_M$, or
$2\mu^{\prime}_1\le M$ in the case $G_M=Sp_M$. Here
$\mu^{\prime}=(\mu^{\prime}_{1},\mu^{\prime}_{2},\,\ldots)$ is the partition
conjugate to $\mu$. Let $W_\mu$ be the irreducible polynomial
representation of the group $G_M$ corresponding to $\mu$.
 
Regard $G_N\times G_M$ as a subgroup of $G_{N+M}$.
Then take any irreducible polynomial representation
$W_\lambda$ of the group $G_{N+M}$.
The vector space
$W_{\lambda}(\mu)={\rm Hom}_{\,G_M}( W_\mu, W_\lambda)$
comes with a natural action of the group $G_N$.
Put $n=\lambda_1-\mu_1+\lambda_2-\mu_2+\ldots\,$.
In this article, for any standard Young tableau $\varOmega$ of
skew shape $\lm$ we give a realization of $W_{\lambda}(\mu)$
as a subspace in the $n$-fold tensor product
$(\mathbb{C}^N)^{\bigotimes n}$, compatible with the action of the group $G_N$.
This subspace is determined as the image of a certain linear operator
$F_\varOmega (M)$ on $(\mathbb{C}^N)^{\bigotimes n}$, given by an explicit formula.
 
When $M=0$ and $W_{\lambda}(\mu)=W_\lambda$ is an irreducible representation of
the group $G_N$, we recover the classical realization of $W_\lambda$
as a subspace in the space of all traceless tensors in $(\mathbb{C}^N)^{\bigotimes n}$.
Then the operator $F_\varOmega\(0)$ may be regarded as the analogue
for $G_N$ of the Young symmetrizer, corresponding to the
standard tableau $\varOmega$ of shape $\lambda$.
This symmetrizer is a certain linear operator on
$\CNn$$(\mathbb{C}^N)^{\bigotimes n} $ with the image equivalent to the irreducible
polynomial representation of the complex general linear group
$GL_N$, corresponding to the partition $\lambda$. Even in the case
$M=0$, our formula for the operator $F_\varOmega(M)$ is new.
 
Our results are applications of the representation
theory of the twisted Yangian, corresponding to the
subgroup $G_N$ of $GL_N$. This twisted Yangian
is a certain one-sided coideal subalgebra of the Yangian corresponding
to $GL_N$. In particular, $F_\varOmega(M)$ is an intertwining
operator between certain representations of the twisted Yangian
in $(\mathbb{C}^N)^{\bigotimes n}$.
