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The E6E_6 Restricted Hyperplane Arrangement and its E7E_7 Shadow: Weyl Transport on a Minuscule Bruhat Poset

Saber Ahmed, Mboyo Esole

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Source: arXiv

Published: Sep 9, 2026

arXiv: 2609.10701

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Source abstract

We study the restricted fan cut inside the dual fundamental Weyl chamber by the weights of a 2727-dimensional minuscule representation of E6E_6; the two such representations are dual and give the same arrangement. Only 1111 of the 2727 weights have kernels meeting its interior, and we prove that they determine the entire fan. It has exactly 1414 chambers and 1818 extreme rays, every chamber is a six-dimensional simplicial cone, and we determine all facets, rays, and incidence relations. The chamber count was previously obtained by Diaconescu and Entin; the simplicial structure, extreme rays, and incidence data are new. The geometry of the 2727 lines on a cubic surface then explains and organizes the resulting chamber architecture. We also enumerate all faces, compute both characteristic polynomials---the arrangement is not supersolvable---together with lattice indices and projective chamber volumes, and describe the oriented matroid. Our main result is representation-theoretic. A distinguished 1414-element visible subposet of the minuscule 56\mathbf{56} of E7E_7, defined entirely inside E7E_7, has Hasse diagram equal to the chamber adjacency graph of the E6E_6 arrangement. Three canonical 7+77+7 splittings of it, of types A7A_7, D7D_7, and E7E_7, are the visible traces of Levi-center u(1)\mathfrak{u}(1)-charge decompositions of the 56\mathbf{56} and reproduce the three level-88 decompositions on the E6E_6 side. More strongly, the simple-root labels on its covers, transported by minimal-length coset representatives, recover chamber by chamber all six facets and, globally, the 1111 active weight hyperplanes and the boundary walls of the dual Weyl chamber. Thus the E7E_7 shadow records not merely the chamber graph but, once matched with the independent E6E_6 classification, the full local wall architecture of I(E6,27)I(E_6,\mathbf{27}).

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