Scaffold the 2^(n-2) constraint-floor proposition
Add section 4: define the achievable boundary set Phi(D) of a triangulated disk and state the constraint-floor proposition |Phi(D)| >= 2^(n-2), with the attainment direction proved (fan injectivity) and the lower bound left as a marked gap with strategy. Remark records the zonotope structure and the short-interface concentration of difficulty. Co-Authored-By: Claude Opus 4.8 <noreply@anthropic.com>
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\newlabel{eq:heawood-face-sum-dual}{{3.1}{4}}
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\bibcite{Heawood1898}{1}
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\citation{bauerfeld-nested-tires}
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@@ -441,6 +441,84 @@ $G$ is properly $4$-vertex-colourable.
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%% pigeonhole bound giving $N(k)$; orientation/reversal bookkeeping on
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%% the shared interface.
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\section{The constraint floor}
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\label{sec:constraint-floor}
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A nested substructure constrains its outer interface through the set of
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Heawood boundary sequences it can realise. By the self-similarity of the
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tire decomposition (\cite{bauerfeld-nested-tires}), the region $G_T$
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enclosed by a tire's outer cycle, away from the source, is itself a
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triangulated disk; we record how tightly any such disk can constrain its
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boundary. The bound below depends only on the disk triangulation, not on
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a tire-tree labelling.
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\begin{definition}[Achievable boundary set of a disk]
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\label{def:achievable-boundary-set}
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Let $D$ be a triangulated disk whose boundary is a simple $n$-cycle
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$C = (v_0, \dots, v_{n-1})$. Call a Heawood face-labelling
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$\lambda : F(D) \to \{+1,-1\}$ \emph{interior-valid} if
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$\sum_{f \ni w} \lambda(f) \equiv 0 \pmod 3$ at every interior vertex $w$
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of $D$ (no condition on $C$). The \emph{achievable boundary set} of $D$
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is
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\[
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\Phi(D) \;:=\; \bigl\{\,
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(\lambda^{*}(v_0), \dots, \lambda^{*}(v_{n-1}))
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\;:\; \lambda \text{ interior-valid} \,\bigr\}
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\;\subseteq\; \{0,1,-1\}^{n} .
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\]
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\end{definition}
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\begin{proposition}[Constraint floor]
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\label{prop:constraint-floor}
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For every triangulated disk $D$ with boundary an $n$-cycle,
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\[
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|\Phi(D)| \;\ge\; 2^{\,n-2},
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\]
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and the bound is attained --- already by the triangulation of the
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$n$-gon with no interior vertices. Consequently no nested structure
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constrains the outer cycle below $2^{\,n-2}$ achievable Heawood
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sequences; the trivial tire is already maximally constraining.
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\end{proposition}
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\begin{proof}[Proof of attainment]
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Triangulate the $n$-gon as a fan from $v_0$, with faces
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$\{v_0, v_i, v_{i+1}\}$ for $1 \le i \le n-2$ and labels
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$\lambda_i := \lambda(\{v_0, v_i, v_{i+1}\})$; there are no interior
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vertices, so every labelling is interior-valid. The induced boundary
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values are
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\[
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\lambda^{*}(v_1) = \lambda_1, \quad
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\lambda^{*}(v_i) = \lambda_{i-1} + \lambda_i \ \ (1 < i < n-1), \quad
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\lambda^{*}(v_{n-1}) = \lambda_{n-2}, \quad
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\lambda^{*}(v_0) = \textstyle\sum_{j} \lambda_j .
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\]
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From $\lambda^{*}(v_1)$ and the relations
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$\lambda_i = \lambda^{*}(v_i) - \lambda_{i-1}$ the tuple
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$(\lambda_1, \dots, \lambda_{n-2}) \in \{+1,-1\}^{n-2}$ is recovered from
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the boundary sequence, so the map $\lambda \mapsto \lambda^{*}|_C$ is
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injective and $|\Phi(D)| = 2^{\,n-2}$.
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\end{proof}
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%% TODO (lower bound): show |Phi(D)| >= 2^{n-2} for EVERY triangulated
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%% disk D. Strategy: the n boundary-incident faces (one per boundary edge)
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%% carry n-2 independent binary degrees of freedom after the interior
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%% Heawood constraints are imposed; those constraints relate only
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%% interior-incident faces and cannot collapse the boundary freedom below
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%% 2^{n-2}. (See notes/boundary_restriction_structure.tex.)
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\begin{remark}
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\label{rem:floor-consequences}
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Two consequences. First, $\Phi(D)$ is a $\mathbb{Z}/3$ zonotope --- a
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projected cube, sign-closed but not a $\mathrm{GF}(3)$ subspace --- and at
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the floor it has size $2^{\,n-2}$ with affine hull of dimension $n-2$.
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Second, since the floor is exponential in the interface length $n$, a
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maximally-constraining child still offers $2^{\,n-2}$ outer options, so
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the gluing of Conjecture~\ref{conj:heawood-chain-pigeonhole} has the least
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slack at \emph{short} interfaces (e.g.\ $n = 4$ leaves $4$ options) and is
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easy at long ones; the difficulty of the programme is concentrated at
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short level cycles.
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\end{remark}
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\begin{thebibliography}{9}
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\bibitem{Heawood1898}
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