Abstract
The Wall Deletion note promoted the chamber decomposition of Twistor Configuration Geometry (TCG) to a full type- Weyl-arrangement structure (postulate ) and showed that a single wall deletion at stratum — the parabolic Levi reduction induced by deleting one simple root from the Dynkin diagram — lands at the Pati–Salam color subalgebra provided the deletion is at an end node; the center node instead gives . That note pre-registered, as its principal open question (Q2), what within TCG selects which simple root to delete?
This note supplies a candidate selection principle. We organize the three single-node deletions as the sectors of a wall-selection functional and show: (i) the bare Weyl-arrangement data admit several inequivalent natural invariants that do not agree on a single deletion — the gauge-level analog of the order-parameter ambiguity of the substrate obstruction theorem — so no selection principle is forced by alone; (ii) conditional on a minimal-breaking (maximal-residual-symmetry) self-energy ansatz, the end-node deletion is selected uniquely up to charge conjugation.
The three wall deletions
| delete | charges on | Levi | broken gens | |
|---|---|---|---|---|
The end-node generator is proportional to the Pati–Salam generator; the end nodes are exchanged by charge conjugation (the same color breaking). The center node is the inequivalent left–right breaking.
Minimal breaking selects the end node
Bare does not force a selector: the cubic anomaly on the favors the center node (), while the broken-generator count favors the end nodes (). Conditional on a minimal-breaking self-energy ansatz with — a standard maximal-little-group heuristic in the Michel stratification of spontaneous symmetry breaking, though not forced (different invariant potentials can select different little groups) — the end-node orbit carries the minimal self-energy and is selected.
The natural invariants split into two classes. Wall-self-energy criteria (minimal broken-generator count, maximal residual symmetry, minimal Richardson orbit ) all select the end node; canonicity / representation / consistency criteria (diagram-automorphism fixedness, self-duality of , balanced branching, vanishing cubic anomaly) favor the center. The anomaly entry is genuinely physical but is not a self-energy of the wall-deletion sector; a dynamical, energy-minimizing functional selects the Pati–Salam end node.
What is and isn’t closed
The result is gauge-arc-internal and conditional, not forced — minimal breaking is a supplied ansatz, and the competing center-node selectors are exhibited explicitly. The selection lands at the Pati–Salam color subalgebra, not the full Standard Model: the missing / hypercharge is untouched. The deeper action-level residual of the Pure-Spinor Condensation Obstruction — which pure-spinor polarization representative the condensate selects — is orthogonal to Q2 and remains open. The configurable-universe reading is preserved unchanged.
Verdict
Conditional-closure construction note — conditional closure of the wall-selection question Q2 of the Wall Deletion note via a minimal-breaking principle; the Pati–Salam end-node deletion is selected uniquely up to charge conjugation; the closure is conditional, not forced. No new postulate and no new active-ledger residual are introduced; the maturity register is that of the AHS substrate closure. The natural upgrade is to derive the minimal-breaking energetics from the active ledger, which would turn the conditional selection into a forced one.
Active TCG/τCG postulate ledger UNCHANGED:
Download paper (Zenodo) — 10 pages, 10 references. CC-BY-4.0.