Virtual-crystal realization conjecture for the four affine types

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Let 4g44\mathfrak{g}4 be of type Dn+1(2)D_{n+1}^{(2)}, A2n(2)A_{2n}^{(2)}, A2n(2)†A_{2n}^{(2)\dagger}, or Cn(1)C_n^{(1)}, let 1≤r≤n1\leq r\leq n and s≥1s\geq1, and let Vr,sV^{r,s} be the virtual crystal with extremal vector u(Vr,s)u(V^{r,s}). Let 4μi44\mu_i4 be defined by 4μn=244\mu_n=24 for 4g=A2n(2)†44\mathfrak{g}=A_{2n}^{(2)\dagger}4 and 4μi=144\mu_i=14 otherwise. Virtual-crystal identification conjecture. Vr,sV^{r,s} is the simple crystal Br,sB^{r,s} of the Uq′(g)U'_q(\mathfrak{g})-module Ws(r)W^{(r)}_s, with extremal vector u(Vr,s)=u(V^r,s)u(V^{r,s})=u(\widehat{V}^{r,s}) of weight sμrΛ‾rs\mu_r\overline{\Lambda}_r; consequently it has the prescribed Uq(g‾)U_q(\overline{\mathfrak{g}})-decomposition and intrinsic energy DVr,s=DBr,sD_{V^{r,s}}=D_{B^{r,s}}. This is the central conjectural identification behind the virtual-crystal construction; the paper proves related statements in special cases but does not establish it uniformly for all listed types and parameters.

References

Primary source

Masato Okado, Anne Schilling and Mark Shimozono, “Virtual crystals and fermionic formulas of type D_n+1^(2), A_2n^(2), and C_n^(1)”, arXiv:math/0105017 (2001).

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