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A cross-boundary right-translation collision propagates to the next point of the left orbit

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FiniteMagmaE677.cross_boundary_collision_propagates_to_left_successor

by mysticflounder · Sep 11, 2026 · Mathlib 0df444a (Lean v4.33.1)

e255e677equational-theoriesfinite-magmaorbit

Fix an element xxx and let Ox={Lxn(x):n≥0}O_x=\{L_x^n(x):n\ge 0\}Ox​={Lxn​(x):n≥0} be its orbit under the left translation Lx(z)=x⋄zL_x(z)=x\diamond zLx​(z)=x⋄z. Assume E677, assume that xxx has no fixer, and assume that AAA is the unique element outside OxO_xOx​. For an orbit element ccc, prove

c⋄x=A⋄x⟹(x⋄c)⋄x=A⋄x.c\diamond x=A\diamond x \quad\Longrightarrow\quad (x\diamond c)\diamond x=A\diamond x.c⋄x=A⋄x⟹(x⋄c)⋄x=A⋄x.

Thus, in the no-fixer branch, a collision between ccc and AAA under right translation by xxx propagates from ccc to the next point x⋄cx\diamond cx⋄c of the left orbit. No associativity, commutativity, or identity is assumed.

Preamble
import Definitions.Def_FiniteMagmaE677

universe u
Formal statement
theorem FiniteMagmaE677.cross_boundary_collision_propagates_to_left_successor
    {α : Type u} [Fintype α] (op : α → α → α) (h : FiniteMagmaE677.E677 op)
    (x A : α)
    (hnofix : ¬ FiniteMagmaE677.HasFixerAt op x)
    (hA_notin : ¬ FiniteMagmaE677.InLeftOrbit op x A)
    (hA_unique : ∀ a : α, ¬ FiniteMagmaE677.InLeftOrbit op x a → a = A)
    (c : α) (hc : FiniteMagmaE677.InLeftOrbit op x c)
    (hcollision : op c x = op A x) :
    op (op x c) x = op A x := by sorry
Source
Local propagation sub-goal isolated from the cross-boundary collision residual in the authors' closure plan (Adam McKenna, The Missing Pair, private repository: docs/current/e677-closure-plan-2026-08-04.md, section 3, and docs/current/spine-refactoring-audit-2026-09-07.md, section 2); Equational Theories Project blueprint, Chapter 13; Bolan et al., arXiv:2512.07087v2, Section 8, Problem 8.1.

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