Add Heawood boundary-restriction experiments and findings note
Experiments probing the cluster restriction set R_K / Phi: R_K is a Z/3 zonotope (not a GF(3) subspace), the "richness" invariant is an artifact of non-shrinking annuli, the interface gluing always works on interior cycles (forced by 4CT), and the maximal constraint achievable on an n-cycle is a floor of 2^(n-2) -- already reached by the trivial tire. Note boundary_restriction_structure.tex writes these up. Co-Authored-By: Claude Opus 4.8 <noreply@anthropic.com>
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\documentclass[11pt]{article}
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\title{Heawood boundary restriction sets:\\
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zonotope structure and the $2^{n-2}$ constraint floor}
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\author{}
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\date{}
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\newtheorem*{obs}{Observation}
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\begin{document}
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\maketitle
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This note records the empirical structure of the Heawood boundary
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restriction sets studied in \texttt{paper.tex}, and a clean
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\emph{maximal-constraint} result. All claims below are backed by the
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experiments in \texttt{experiments/} (filenames given inline). Sequences
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live in $(\mathbb{Z}/3)^{\,\cdot}$, displayed in $\{0,1,-1\}$.
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\section*{Setup}
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Fix a triangulated disk $D$ with boundary cycle $C = (v_0,\dots,v_{n-1})$.
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A Heawood face-labelling is $\lambda : \{\text{faces of }D\} \to \{+1,-1\}$,
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with induced vertex value $\lambda^{*}(v) = \sum_{f \ni v}\lambda(f) \bmod 3$.
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The achievable outer set is
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\[
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\Phi(D) \;=\; \bigl\{\, (\lambda^{*}(v_0),\dots,\lambda^{*}(v_{n-1}))
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\;:\; \lambda \in \{+1,-1\}^{F(D)},\;
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\lambda^{*}(w) \equiv 0 \ \forall\ \text{interior } w \,\bigr\}.
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\]
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This is exactly the value the recursive transfer operator produces at
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$C$ (interior consistency $=$ all descendant gluings performed; boundary
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deferred). Crucially $\Phi(D)$ depends \emph{only} on the disk
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triangulation, not on any BFS/tire-tree labelling.
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\section*{1. The restriction sets are zonotopes, not subspaces}
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(\texttt{probe\_RK\_structure.py}.) Writing $\lambda = \mathbf{1}+b$ with
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$b \in \{0,1\}^F$, the labelling map is $\lambda \mapsto M\mathbf{1}+Mb
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\pmod 3$, a linear image of the Boolean cube ($M$ the face/vertex
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incidence matrix). Over $3655$ cluster restriction sets $R_{\mathsf K}$:
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none was an affine $\mathrm{GF}(3)$ subspace; the map is usually
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injective, so $|R_{\mathsf K}| = 2^{|F|}$ (a power of $2$ inside the
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column space of size $3^{\operatorname{rank} M}$); the nowhere-zero
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constraint $\lambda \neq 0$ shrank the set below the full linear image in
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\emph{every} case. The only surviving linear structure is
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$R_{\mathsf K} \subseteq \operatorname{col}(M)$ (cokernel relations such
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as $\sum_v \lambda^{*}(v) \equiv 0$). So $\Phi$ is a $\mathbb{Z}/3$
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zonotope: a projected cube, sign-closed but not closed under addition.
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\section*{2. ``Richness'' is not a self-similar invariant}
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(\texttt{transfer\_operator.py}, \texttt{branch\_invariant.py}.) In a
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homogeneous same-$n$ spoke-only chain the operator saturates: $\Phi$ has
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full single-position marginals (every interface vertex independently
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attains all of $\{0,1,-1\}$), and the alternating tire reaches the
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\emph{entire} space $3^n$. This is an artifact of non-shrinking annuli
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with no interior constraints. On genuine triangulations the marginal
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fullness holds for only ${\sim}8\%$ of regions: depth (not branching)
|
||||
shrinks $\Phi$, e.g.\ a region with $|C|=10$ realised only $|\Phi|=400$
|
||||
of $3^{10}\approx 59000$. Only non-emptiness and sign-closure survive,
|
||||
both of which are automatic / equivalent to $4$CT. Hence no abundance
|
||||
(counting) pigeonhole: a working invariant must tolerate \emph{small}
|
||||
$\Phi$.
|
||||
|
||||
\section*{3. The maximal-constraint floor}
|
||||
|
||||
(\texttt{maximally\_constrain.py}.) Minimising $|\Phi(D)|$ over disks with
|
||||
a fixed boundary $n$-cycle:
|
||||
|
||||
\begin{center}
|
||||
\begin{tabular}{ccccc}
|
||||
\toprule
|
||||
$n$ & $4$ & $5$ & $6$ & $7$\\
|
||||
\midrule
|
||||
$\min |\Phi|$ (search) & $4$ & $8$ & $16$ & $32$\\
|
||||
fan, $0$ interior vertices & $4$ & $8$ & $16$ & $32$\\
|
||||
$2^{\,n-2}$ & $4$ & $8$ & $16$ & $32$\\
|
||||
\bottomrule
|
||||
\end{tabular}
|
||||
\end{center}
|
||||
|
||||
A search over random and deep-stacked disks (up to $8$ interior vertices)
|
||||
never beat $2^{n-2}$, and the interior-free triangulation already
|
||||
attains it. Thus:
|
||||
|
||||
\begin{obs}
|
||||
The outer $n$-cycle cannot be constrained below $2^{n-2}$ achievable
|
||||
sequences, and no nested structure is needed to reach the floor: a single
|
||||
trivial tire is already maximal. Deep nesting only approaches the floor
|
||||
from above.
|
||||
\end{obs}
|
||||
|
||||
The achievability is transparent: in a fan from $v_0$,
|
||||
\[
|
||||
\sigma_1 = \lambda_1,\quad
|
||||
\sigma_i = \lambda_{i-1}+\lambda_i \ (1<i<n-1),\quad
|
||||
\sigma_{n-1} = \lambda_{n-2},\quad
|
||||
\sigma_0 = \textstyle\sum_j \lambda_j ,
|
||||
\]
|
||||
so $(\lambda_1,\dots,\lambda_{n-2})$ is recoverable from $\sigma$ and the
|
||||
map is injective onto $2^{n-2}$ sequences. The lower bound over
|
||||
\emph{all} disks is the substance:
|
||||
|
||||
\begin{conj}[Boundary degrees of freedom]
|
||||
For every triangulated disk $D$ with boundary $n$-cycle,
|
||||
$|\Phi(D)| \ge 2^{n-2}$. Equivalently, the $n-2$ binary degrees of
|
||||
freedom carried by the boundary-incident faces survive every interior
|
||||
Heawood constraint (which relates only interior-incident faces).
|
||||
\end{conj}
|
||||
|
||||
The minimal set is itself a sign-closed zonotope of size $2^{n-2}$, hull
|
||||
dimension $n-2$, not a $\mathrm{GF}(3)$ subspace --- the same fingerprint
|
||||
as $\S1$.
|
||||
|
||||
\section*{Consequence for the pigeonhole}
|
||||
|
||||
Even a maximally-constraining child still presents $2^{n-2}$ outer
|
||||
options --- exponential in the interface length $n$. So the gluing
|
||||
problem has the least slack at \emph{short} interfaces ($n=4$ leaves $4$
|
||||
options, $n=3$ leaves $2$), and is easy at long ones. The crux of the
|
||||
Heawood programme therefore lives entirely at short level cycles, exactly
|
||||
where the medial programme's $N(k)$ bound concentrates.
|
||||
|
||||
\medskip
|
||||
\noindent\emph{Meta-remark.} Because $4$CT holds, every actual
|
||||
triangulation glues, so no experiment can exhibit an obstruction (pair or
|
||||
chain). The experiments measure \emph{structure} (zonotope type,
|
||||
constraint floor), not proof difficulty; the difficulty is localised, not
|
||||
removed.
|
||||
|
||||
\end{document}
|
||||
Reference in New Issue
Block a user