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Let be a quantized (-theoretic) BFN Coulomb branch with and any , that is, is a generalized Weyl or -Weyl algebra. Let be an - bimodule. Choosing an automorphism of we can define the notion of an invariant Hermitian form: for all and . We obtain a classification of invariant positive definite forms on in the case when is Harish-Chandra in the sense of Losev and quantization parameter is generic.

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