Symmetry conjecture for the two-factor fermionic sum

Let g\mathfrak g be a Kac–Moody algebra, let β\beta be a positive-root-lattice element, and let Xβλ1,λ2X^{\lambda_1,\lambda_2}_\beta be the bilinear fermionic quantity defined from the corresponding vectors. For ADE type, the source identifies it with XC,m(0,ν)(q,z)X^{(0,\nu)}_{C,m}(q,z) and proves Xβλ1,λ2=Xβλ2,λ1X^{\lambda_1,\lambda_2}_\beta=X^{\lambda_2,\lambda_1}_\beta. Two-factor symmetry conjecture. The relation

Xβλ1,λ2=Xβλ2,λ1X^{\lambda_1,\lambda_2}_\beta=X^{\lambda_2,\lambda_1}_\beta

holds for arbitrary g\mathfrak g. The claim extends the equality proved in the ADE case to arbitrary Lie type. The excerpt gives no proof for the general case, so its status is open.

Sources & referencesView supporting material

Primary source

B. Feigin, E. Feigin, M. Jimbo, T. Miwa and E. Mukhin, “Fermionic formulas for eigenfunctions of the difference Toda Hamiltonian”, arXiv:0812.2306 (2018).

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