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Electrical Networks and Symplectic Invariants

David Kogan

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Source: arXiv

Published: Oct 6, 2026

arXiv: 2610.07539

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Source abstract

Consider a finite planar graph with positive real edge weights and designated boundary vertices, called nodes. Such a graph is called a circular planar electrical network. A grove is a spanning forest in which every component contains at least one node. The connected components of a grove determine a partition of the nodes. We relate weighted grove counts to invariant theory for the symplectic group. To a planar electrical network GG, we associate an Sp(2n)\mathrm{Sp}(2n)-invariant tensor ZGZ_G. For Sp(2)=SL(2)\mathrm{Sp}(2)=\mathrm{SL}(2), we expand ZGZ_G in the Temperley--Lieb basis indexed by noncrossing matchings and relate its coefficients to the Kenyon--Wilson grove formulas. For Sp(4)\mathrm{Sp}(4), we give reduction rules for superpositions of two groves and prove that the tensors indexed by 33-noncrossing matchings form a basis of the space of Sp(4)\mathrm{Sp}(4)-invariant tensors. The coefficients of ZGZ_G in this basis are weighted counts of reduced double groves, up to normalization.

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