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In this paper, we consider the restriction of finite dimensional $GL_{mn}(\C)$-modules to the subgroup ${GL_m (\C)\times GL_n (\C)}$. In particular, fora Weyl module $V_{\lambda} (\C^{mn})$ of $U_q(gl_{mn})$ we construct arepresentation $W_{\lambda}$ of $U_q (gl_m)\otimes U_q (gl_n)$ such that at$q=1$, the restriction of $V_{\lambda} (\C^{mn})$ to $U_1 (gl_m)\otimes U_1(gl_n)$ matches its action on $W_{\lambda}$ at $q=1$. Thus $W_{\lambda}$ is a$q$-deformation of the module $V_{\lambda}$. This is achieved by firstconstructing a $U_q (gl_m)\otimes U_q (gl_n)$-module $\wedge^k $, a$q$-deformation of the simple $GL_{mn} (\C)$-module $\wedge^k (\C^{mn})$. Wealso construct the bi-crystal basis for $\wedge^k $ and show that it consistsof signed subsets. Next, we develop $U_q (gl_m) \otimes U_q (gl_n)$-equivariantmaps $\psi_{a,b} :\wedge^{a+1} \otimes \wedge^{b-1} \to \wedge^a \otimes\wedge^b$. This is used as the building block to construct the general$W_{\lambda}$.

Quantum deformations of the restriction of $GL_{mn}(\C)$-modules to $GL_m(\C) \times GL_n(\C)$