Gaudin monodromy conjectures for crystal tensor products

Let g\mathfrak{g} be a simple Lie algebra, let V(λ1),,V(λn)V(\lambda_1),\ldots,V(\lambda_n) be irreducible representations, write V(λ)=V(λ1)V(λn)V({\underline{\lambda}})=V(\lambda_1)\otimes\cdots\otimes V(\lambda_n), and let V(λ)μV({\underline{\lambda}})_\mu denote its μ\mu-weight space. Let B(λi)B(\lambda_i) be the normal crystal of highest weight λi\lambda_i, and let vCn=π1Sn(Fn(R))vC_n=\pi_1^{S_n}(\overline F_n(\mathbb{R})), Cn~=π1Sn(Mn+2split(R))\widetilde{C_n}=\pi_1^{S_n}(\overline M_{n+2}^{split}(\mathbb{R})), and AC~n=π1Sn(Mn+2comp(R))\widetilde{AC}_n=\pi_1^{S_n}(\overline M_{n+2}^{comp}(\mathbb{R})). The inhomogeneous and trigonometric Gaudin Hamiltonians have corresponding eigenlines in V(λ)μV({\underline{\lambda}})_\mu. Gaudin monodromy conjectures. (1) The monodromy action of vCnvC_n on the inhomogeneous Gaudin eigenlines in V(λ)μV({\underline{\lambda}})_\mu matches the action of vCnvC_n on B(λ1)B(λn)B(\lambda_1)\otimes\cdots\otimes B(\lambda_n) given by crystal commutors and naive permutation of tensor factors. (2) The monodromy action of Cn~\widetilde{C_n} on the trigonometric Gaudin eigenlines in V(λ)μV({\underline{\lambda}})_\mu factors surjectively through the action of vCnvC_n. (3) The monodromy action of AC~n\widetilde{AC}_n on the trigonometric Gaudin eigenlines in V(λ)μV({\underline{\lambda}})_\mu factors through the action of vCnvC_n and is given by crystal commutors and cyclic rotation of tensor factors. These conjectures relate monodromy of Gaudin eigenlines to the combinatorial actions on tensor products of crystals; the source says they are intended to be proved in future work, so their resolution is not established here.

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Primary source

Aleksei Ilin, Joel Kamnitzer and Leonid Rybnikov, “Gaudin models and moduli space of flower curves”, arXiv:2407.06424 (2025).

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