Two Wilson loop diagrams define the same positroid exactly when they differ by retriangulating certain exact subdiagrams, and inequivalent diagrams correspond to non-parallel faces of an associahedron.
A study in $\mathbb{G}_{\mathbb{R}, \geq 0}$: from the geometric case book of Wilson loop diagrams and SYM $N=4$
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abstract
We study the geometry underlying the Wilson loop diagram approach to calculating scattering amplitudes in the gauge theory of Supersymmetric Yang Mills (SYM) $N=4$. By applying the tools developed to study total positivity in the real Grassmannian, we are able to systematically compute with all Wilson loop diagrams of a given size and find unexpected patterns and relationships between them. We focus on the smallest nontrivial multi-propagator case, consisting of 2 propagators on 6 vertices, and compute the positroid cells associated to each diagram and the homology of the subcomplex they generate in $\mathbb{G}_{\mathbb{R}, \geq 0}$. We also verify in this case the conjecture that the spurious singularities of the volume functional {\em do} all cancel on the codimension 1 boundaries of these cells.
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Combinatorics of the geometry of Wilson loop diagrams I: equivalence classes via matroids and polytopes
Two Wilson loop diagrams define the same positroid exactly when they differ by retriangulating certain exact subdiagrams, and inequivalent diagrams correspond to non-parallel faces of an associahedron.