Run Heawood pigeonhole between nested connected tire clusters
Add the two-sided cluster decomposition proposition: a vertex's full Heawood face-sum splits as exactly one child-cluster contribution plus one parent-cluster contribution (the at-most-two-clusters bound makes the pairing binary and complete). Explain why this fails per-tire -- a vertex on many same-depth tires has only a fragment of its face-star in any one tire -- and recast the chain-pigeonhole and 4CT conjectures to nested clusters with a cluster restriction relation. Co-Authored-By: Claude Opus 4.8 <noreply@anthropic.com>
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\newlabel{rem:no-interior-constraint}{{3.2}{3}}
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\newlabel{def:boundary-sequences}{{3.3}{3}}
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\newlabel{def:heawood-compatible}{{3.4}{3}}
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\newlabel{rem:compat-is-heawood}{{3.5}{4}}
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\newlabel{eq:heawood-face-sum-dual}{{3.1}{4}}
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\@writefile{toc}{\contentsline {subsection}{\tocsubsection {}{}{Why the programme runs between nested clusters}}{4}{}\protected@file@percent }
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\newlabel{prop:two-sided-decomposition}{{3.6}{4}}
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\bibcite{Heawood1898}{1}
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\bibcite{bauerfeld-depth}{2}
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\bibcite{bauerfeld-nested-tires}{3}
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\bibcite{bauerfeld-medial-tires}{4}
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\bibcite{bauerfeld-nested-tire-duals}{5}
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\newlabel{rem:compat-is-heawood}{{3.5}{4}}
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@@ -303,34 +303,130 @@ $\{+1,-1\}$ face-labelling of $G$ satisfying
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proper $4$-vertex-colouring of $G$.
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\end{remark}
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\subsection*{Why the programme runs between nested clusters}
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The vanishing condition \eqref{eq:heawood-face-sum-dual} at a vertex $v$
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is a constraint on the \emph{full} face-star of $v$. To run a
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pigeonhole between two objects --- a child and a parent --- we need that
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full sum to split as exactly two one-sided contributions, so that each
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vertex label is the combination of a single child value and a single
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parent value. This is true at the level of connected tire clusters, and
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\emph{false} at the level of individual tires. Extend a Heawood
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face-labelling to a connected tire cluster $\mathsf{K}$ by labelling
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every annular face of every tire of $\mathsf{K}$, and for $v \in
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V(\mathsf{K})$ write
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\[
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\lambda^{\!*}_{\mathsf{K}}(v) \;:=\;
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\sum_{f} \lambda(f) \;\bmod 3,
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\]
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the sum over the annular faces of $\mathsf{K}$ incident to $v$.
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\begin{proposition}[Two-sided cluster decomposition at a vertex]
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\label{prop:two-sided-decomposition}
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Let $v \in V(G)$ have level $\ell = \ell_G(v)$, and let
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$\mathsf{K}_{\ell}$ and $\mathsf{K}_{\ell-1}$ be the at most two
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connected tire clusters containing $v$, of depths $\ell$ and $\ell-1$
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respectively (Proposition~\ref{prop:two-clusters-per-vertex}). Then the
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bounded faces of $G$ incident to $v$ partition into the annular faces of
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$\mathsf{K}_{\ell}$ at $v$ and the annular faces of $\mathsf{K}_{\ell-1}$
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at $v$, and
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\[
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\sum_{f \ni v} \lambda(f)
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\;\equiv\;
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\lambda^{\!*}_{\mathsf{K}_{\ell}}(v) +
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\lambda^{\!*}_{\mathsf{K}_{\ell-1}}(v)
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\pmod 3 .
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\]
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Each one-sided value $\lambda^{\!*}_{\mathsf{K}_d}(v)$ is the
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\emph{complete} sum over all depth-$d$ faces at $v$, so the Heawood
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condition \eqref{eq:heawood-face-sum-dual} at $v$ reads
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\[
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\lambda^{\!*}_{\mathsf{K}_{\ell}}(v) +
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\lambda^{\!*}_{\mathsf{K}_{\ell-1}}(v) \;\equiv\; 0 \pmod 3 ,
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\]
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a pairing between the single child cluster $\mathsf{K}_{\ell}$ and the
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single parent cluster $\mathsf{K}_{\ell-1}$. (When $\ell = 0$, or when
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$v$ bounds no depth-$\ell$ face, only one term is present.)
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\end{proposition}
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\begin{proof}
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By Proposition~\ref{prop:two-clusters-per-vertex} (Step~1) every bounded
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face incident to $v$ has depth $\ell-1$ or $\ell$, partitioning the
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incident faces by depth; by Step~2 all depth-$\ell$ faces at $v$ lie in
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the single cluster $\mathsf{K}_{\ell}$ and all depth-$(\ell-1)$ faces at
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$v$ in $\mathsf{K}_{\ell-1}$. Hence the depth-$\ell$ part is exactly the
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annular faces of $\mathsf{K}_{\ell}$ at $v$, the depth-$(\ell-1)$ part
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those of $\mathsf{K}_{\ell-1}$, and summing $\lambda$ over the two parts
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gives the identity; \eqref{eq:heawood-face-sum-dual} is its vanishing.
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\end{proof}
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\begin{remark}[Failure at the tire level]
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\label{rem:why-clusters}
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Proposition~\ref{prop:two-sided-decomposition} is what makes the binary
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parent/child pairing possible, and it requires the cluster. A vertex
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$v$ may lie on many depth-$\ell$ tires --- the unbounded case of
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Section~\ref{sec:tire-clusters} --- and the per-tire value
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$\lambda^{\!*}(v)$ of Definition~\ref{def:heawood-labelling} then records
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only the faces of \emph{one} tire at $v$, a fragment of $v$'s face-star.
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No single child tire carries the complete depth-$\ell$ sum, so the label
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$\sum_{f \ni v}\lambda(f)$ cannot be written as one child value plus one
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parent value, and per-tire compatibility
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(Definition~\ref{def:heawood-compatible}) fails to assemble to
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\eqref{eq:heawood-face-sum-dual}. Clustering repairs this:
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Proposition~\ref{prop:two-clusters-per-vertex} guarantees exactly one
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cluster meets $v$ on each side, so $\lambda^{\!*}_{\mathsf{K}_{\ell}}(v)$
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is the complete child contribution and
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$\lambda^{\!*}_{\mathsf{K}_{\ell-1}}(v)$ the complete parent
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contribution. Every vertex label is then realised as the combination of
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a single child-cluster value with a single parent-cluster value, and the
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pigeonhole programme below chains \emph{nested connected tire clusters}
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rather than individual tires.
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\end{remark}
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We write $R_{\mathsf{K}}$ for the \emph{cluster Heawood restriction
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relation}: the set of (outer, inner) boundary Heawood sequence pairs
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realisable by a face-labelling of $\mathsf{K}$, defined as in
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Definition~\ref{def:boundary-sequences} but with the outer and inner
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boundaries of the cluster and the complete one-sided values
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$\lambda^{\!*}_{\mathsf{K}}$ in place of a single tire's, read up to
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rotation and global sign-flip. By
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Proposition~\ref{prop:two-sided-decomposition} two nested clusters are
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compatible along their shared interface exactly when the inner sequence
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of the parent is the pointwise negation mod $3$ of the outer sequence of
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the child (after the orientation reversal of
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Definition~\ref{def:heawood-compatible}).
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\begin{conjecture}[Heawood chain-pigeonhole principle]
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\label{conj:heawood-chain-pigeonhole}
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There is a function $N(k)$ such that the following holds. Let
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\[
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T_0 \supset T_1 \supset \cdots \supset T_{N(k)}
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\mathsf{K}_0 \supset \mathsf{K}_1 \supset \cdots \supset
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\mathsf{K}_{N(k)}
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\]
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be a nested chain of tires in $\mathcal{T}(G, S)$ whose shared interface
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cycles have length at most $k$. Then two adjacent Heawood restriction
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relations $R_{T_i}, R_{T_{i+1}}$ in the chain admit compatible
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face-labellings along their shared interface
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(Definition~\ref{def:heawood-compatible}), after rotation and global
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sign-flip. Equivalently, the chain contains a local gluing step that
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cannot be obstructed by disjoint Heawood boundary restrictions.
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be a nested chain of connected tire clusters in $\mathcal{T}(G, S)$ whose
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shared interfaces have length at most $k$. Then two adjacent cluster
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restriction relations $R_{\mathsf{K}_i}, R_{\mathsf{K}_{i+1}}$ in the
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chain admit compatible face-labellings along their shared interface,
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after rotation and global sign-flip. Equivalently, the chain contains a
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local gluing step that cannot be obstructed by disjoint Heawood boundary
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restrictions.
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\end{conjecture}
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\begin{conjecture}[Heawood tire route to the Four Colour Theorem]
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\begin{conjecture}[Heawood cluster route to the Four Colour Theorem]
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\label{conj:heawood-route-fct}
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For every plane triangulation $G$ and every level source $S$, the
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Heawood restriction relations $\{R_T : T \in \mathcal{T}(G, S)\}$ admit
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a selection of face-labellings that is compatible along every interface
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of the tire tree. By Remark~\ref{rem:compat-is-heawood} this yields a
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$\{+1,-1\}$ face-labelling of $G$ satisfying
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\eqref{eq:heawood-face-sum-dual}, hence $G$ is properly
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$4$-vertex-colourable.
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cluster Heawood restriction relations
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$\{R_{\mathsf{K}} : \mathsf{K} \text{ a connected tire cluster}\}$ admit
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a selection of face-labellings that is compatible along every cluster
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interface. By Proposition~\ref{prop:two-sided-decomposition} and
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Remark~\ref{rem:compat-is-heawood} this yields a $\{+1,-1\}$
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face-labelling of $G$ satisfying \eqref{eq:heawood-face-sum-dual}, hence
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$G$ is properly $4$-vertex-colourable.
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\end{conjecture}
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%% TODO: realisability of $R_T$ per tire; counting / pigeonhole bound
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%% giving $N(k)$; orientation/reversal bookkeeping on $\gamma$.
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%% TODO: realisability of $R_{\mathsf{K}}$ per cluster; counting /
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%% pigeonhole bound giving $N(k)$; orientation/reversal bookkeeping on
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%% the shared interface.
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\begin{thebibliography}{9}
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