Tensor-product fixed-point conjecture for Coulomb branches

Let W=W1W2W=W^1\oplus W^2 be a decomposition inducing dominant coweights λ1\lambda^1 and λ2\lambda^2, let Mν(λ,μ)\mathcal M^\nu(\lambda,\mu) be the corresponding deformation of the Coulomb branch, and let χ\chi act on it as above. The tensor-product fixed-point conjecture. The fixed-point set Mν(λ,μ)χ\mathcal M^\nu(\lambda,\mu)^\chi is finite and has a natural bijection with

μ=μ1+μ2M(λ1,μ1)χ×M(λ2,μ2)χ.\bigsqcup_{\mu=\mu^1+\mu^2}\mathcal M(\lambda^1,\mu^1)^\chi\times\mathcal M(\lambda^2,\mu^2)^\chi.

Together with the preceding fixed-point and geometric Satake conjectures, this would identify the nonempty fixed-point condition with the condition that μ\mu is a weight of V(λ1)V(λ2)V(\lambda^1)\otimes V(\lambda^2); it is not established in general.

Sources & referencesView supporting material

Primary source

Hiraku Nakajima, “A mathematical definition of Coulomb branches of supersymmetric gauge theories and geometric Satake correspondences for Kac-Moody Lie algebras”, arXiv:2201.08386 (2023).

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