Quiver formula for the extended Goldman Poisson bracket

Following Fock and Goncharov, consider a triangulation Σ0\Sigma_0 and its subtriangulation into sub-triangles, with the associated extended quiver Q\mathscr Q. The nodes of Q\mathscr Q carry the Fock–Goncharov variables and the additional toric variables, and let σ,σ\sigma,\sigma' be the logarithms of any two variables associated with nodes p,pp,p' of this quiver. The symbol ϵp,p\epsilon_{p,p'} is determined by the arrow between the nodes: it is 11 when the arrow goes from pp to pp', 1-1 in the opposite direction, and ±12\pm \frac12 for a dashed arrow. Quiver formula for the extended Goldman Poisson bracket. The Poisson bracket inverse to the extended Goldman symplectic form W\mathcal W satisfies

n2{σ,σ}=ϵp,p.n^2\{\sigma,\sigma'\}=\epsilon_{p,p'}.

In particular, the brackets between Fock–Goncharov variables are given by the original Fock–Goncharov quiver. This extends the usual quiver description of the Goldman structure to the added toric variables associated with cherries; the parser supplies no evidence resolving the assertion, so its status remains open.

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Primary source

Marco Bertola and Dmitry Korotkin, “Extended Goldman symplectic structure in Fock-Goncharov coordinates”, arXiv:1910.06744 (2021).

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