Higher Narayana number formula for local Weyl modules

Let WCd({0}nω)W_{\mathbb C^d}(\{0\}_{n\omega}) be the indicated local Weyl module for sl2sl_2, and let WCd({0}nω)n2iW_{\mathbb C^d}(\{0\}_{n\omega})^{n-2i} denote its weight space of weight n2in-2i. Higher Narayana number conjecture. For i=0,,ni=0,\dots,n, one has

dimWCd({0}nω)n2i=(d+n1)!(d+ni)!(n1)!(ni)!2!(i1)!d!(d+i1)!,\dim W_{\mathbb C^d}(\{0\}_{n\omega})^{n-2i}=\frac{(d+n-1)!\cdots(d+n-i)!}{(n-1)!\cdots(n-i)!}\cdot\frac{2!\cdots(i-1)!}{d!\cdots(d+i-1)!},

and these dimensions equal the dimension of the irreducible representation of slnsl_n with highest weight dωid\omega_i for i=1,,n1i=1,\dots,n-1, while they equal one for i=0,ni=0,n. This proposes a higher-dimensional analogue of the Catalan and Narayana number formulas established earlier in the paper; the source gives no resolution of the proposed formula.

Sources & referencesView supporting material

Primary source

B. Feigin and S. Loktev, “Multi-dimensional Weyl Modules and Symmetric Functions”, arXiv:math/0212001 (2004).

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