%% filename: amsart-template.tex %% American Mathematical Society %% AMS-LaTeX v.2 template for use with amsart %% ==================================================================== \documentclass{amsart} \usepackage{amssymb} \usepackage{graphicx} \newtheorem{theorem}{Theorem}[section] \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \newtheorem{proposition}[theorem]{Proposition} \newtheorem{conjecture}[theorem]{Conjecture} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \newtheorem{example}[theorem]{Example} \newtheorem{xca}[theorem]{Exercise} \theoremstyle{remark} \newtheorem{remark}[theorem]{Remark} \numberwithin{equation}{section} \begin{document} \title{Heawood Restrictions on Nested Tire Graph Duals} % author one information \author{Eric Bauerfeld} \address{} \curraddr{} \email{} \thanks{} \subjclass[2010]{Primary } \keywords{plane graph, triangulation, plane depth, level edge, dual graph, tire graph, Heawood number} \date{} \dedicatory{} \begin{abstract} %% TODO: abstract. Following \cite{bauerfeld-nested-tires}, which establishes %% the basic vocabulary of tire graphs and dual depth, we study the Heawood %% (mod-3 / face-sum) restrictions imposed on the duals of nested tire graphs. \end{abstract} \maketitle \section{Introduction} A classical theorem of Tait recasts the Four Colour Theorem in dual, edge-colouring terms: a plane triangulation $G$ is properly $4$-vertex-colourable if and only if its dual cubic graph $G'$ is properly $3$-edge-colourable. Thus a minimal counterexample to the Four Colour Theorem -- a smallest triangulation admitting no proper $4$-colouring -- corresponds to a smallest cubic plane graph admitting no proper $3$-edge-colouring. This paper continues the series studying that structure through the lens of \emph{nested level duals}. The foundational vocabulary --- level sources, levels, the inner planar dual $G'$ and its dual depth, and tire graphs --- is developed in the companion paper \cite{bauerfeld-nested-tires}; we refer to that paper for those definitions and rely on them throughout. In particular we use, without restating, the notions of: \begin{itemize} \item \emph{level source} $S$ and $G$-vertex levels $\ell_G(v)$; \item the inner planar dual $G'$ (\cite[Definition~1.3]{bauerfeld-nested-tires}); \item \emph{dual depth} $\delta_G(d_f)$ (\cite[Definition~1.4]{bauerfeld-nested-tires}); \item \emph{tire graph} $T = (B_{\mathrm{out}}, O, E_{\mathrm{ann}})$ with outer/inner boundaries and annular edges (\cite[Definition~1.5]{bauerfeld-nested-tires}); \item the \emph{tire-component lemma} (\cite[Lemma~1.8]{bauerfeld-nested-tires}); and \item the \emph{tire-tread partition theorem} (\cite[Theorem~1.9]{bauerfeld-nested-tires}). \end{itemize} Throughout, $G = (V, E)$ is a plane maximal planar graph (a triangulation) with a fixed planar embedding $\Pi_G$. We write $|V| = n$, so $|E| = 3n - 6$ and $G$ has $2n - 4$ triangular faces. The classical input is Heawood's face-sum identity \cite{Heawood1898}: for any proper $3$-edge-colouring of a cubic plane graph $H$, assigning each face of $H$ a number in $\{+1, -1\}$ can be done so that the labels around every vertex of $H$ sum to $0 \pmod 3$. In the triangulation $G$ dual to $H$ this becomes a $\{+1, -1\}$ labelling of the \emph{faces} of $G$ whose incident-face sum at every vertex of $G$ vanishes mod $3$. Our aim is to record what this restriction forces along the boundary cycles of a nested tire graph, and to formulate a chain-pigeonhole programme in this Heawood labelling parallel to the medial programme of \cite{bauerfeld-medial-tires}. \section{Heawood restrictions on the tire dual} \label{sec:heawood-restrictions} We work inside a fixed nested tire decomposition $\mathcal{T}(G, S)$ of $G$ from a single-vertex level source $S$ \cite{bauerfeld-nested-tires}, and use the tire data $T = (B_{\mathrm{out}}, O, E_{\mathrm{ann}})$ with annular faces $F_{\mathrm{ann}}$, outer boundary $B_{\mathrm{out}}$, and inner boundary $B_{\mathrm{in}}$ (\cite[Definition~1.5]{bauerfeld-nested-tires}). Since $O$ is outerplanar, every vertex of a tire lies on $B_{\mathrm{out}}$ or on the inner-boundary walk $B_{\mathrm{in}}$; a tire has no interior vertices. \begin{definition}[Heawood face-labelling of a tire] \label{def:heawood-labelling} A \emph{Heawood face-labelling} of a tire graph $T$ is a map \[ \lambda : F_{\mathrm{ann}} \longrightarrow \{+1, -1\} \] assigning a sign to each annular face of $T$. For a vertex $v \in V(T)$, write $F_{\mathrm{ann}}(v) \subseteq F_{\mathrm{ann}}$ for the set of annular faces of $T$ incident to $v$, and define the \emph{induced vertex value} \[ \lambda^{\!*}(v) \;:=\; \sum_{f \in F_{\mathrm{ann}}(v)} \lambda(f) \;\;\bmod 3 \;\in\; \{0, 1, -1\}. \] The value $\lambda^{\!*}(v)$ is the \emph{partial} face-sum at $v$ taken over the annular faces of $T$ alone, not over all faces of $G$ incident to $v$. \end{definition} \begin{remark} \label{rem:no-interior-constraint} Because a tire has no interior vertices, every annular face of $T$ is incident to $B_{\mathrm{out}} \cup B_{\mathrm{in}}$, and a Heawood face-labelling is subject to \emph{no} internal constraint: all $2^{|F_{\mathrm{ann}}|}$ sign assignments are admissible. The Heawood restriction is felt only on the two boundary cycles, through the induced vertex values $\lambda^{\!*}$. \end{remark} \begin{definition}[Induced boundary sequences] \label{def:boundary-sequences} Let $\lambda$ be a Heawood face-labelling of $T$. Reading the vertices of $B_{\mathrm{out}}$ in clockwise order $v_0, v_1, \dots, v_{p-1}$, the \emph{outer Heawood sequence} of $(T, \lambda)$ is \[ \sigma_{\mathrm{out}}(T, \lambda) \;:=\; \bigl(\lambda^{\!*}(v_0), \dots, \lambda^{\!*}(v_{p-1})\bigr) \;\in\; \{0, 1, -1\}^{p}. \] Reading the inner-boundary walk $B_{\mathrm{in}}$ in clockwise order $w_0, \dots, w_{q-1}$ gives the \emph{inner Heawood sequence} $\sigma_{\mathrm{in}}(T, \lambda) \in \{0, 1, -1\}^{q}$. The \emph{Heawood restriction relation} of $T$ is the set \[ R_T \;:=\; \bigl\{\, \bigl(\sigma_{\mathrm{out}}(T, \lambda),\, \sigma_{\mathrm{in}}(T, \lambda)\bigr) \;:\; \lambda : F_{\mathrm{ann}} \to \{+1, -1\} \,\bigr\} \] of all (outer, inner) sequence pairs realisable by a single face-labelling, read up to rotation and the global sign-flip $\lambda \mapsto -\lambda$ (equivalently $\sigma \mapsto -\sigma$). \end{definition} \begin{definition}[Heawood compatibility across an interface] \label{def:heawood-compatible} Let $T$ be a tire and $T' \in \mathcal{T}(G, S)$ a child of $T$, so the outer boundary cycle $B_{\mathrm{out}}^{(T')}$ coincides with a bounded face of $O^{(T)}$; let $\gamma$ be this shared cycle, of length $L$, and let $v$ range over its vertices. Heawood face-labellings $\lambda$ of $T$ and $\lambda'$ of $T'$ are \emph{compatible along $\gamma$} if at every shared vertex $v$, \[ \lambda^{\!*}(v) + (\lambda')^{\!*}(v) \;\equiv\; 0 \pmod 3, \] i.e.\ $0$ is paired with $0$ and $+1$ with $-1$. Equivalently, the inner Heawood sequence of $T$ on $\gamma$ is the pointwise negation mod $3$ of the outer Heawood sequence of $T'$ on $\gamma$, after reversing one of the two clockwise readings to account for the opposite rotational senses in which $T$ and $T'$ traverse $\gamma$. \end{definition} \begin{remark} \label{rem:compat-is-heawood} Compatibility along $\gamma$ at $v$ is exactly the statement that the full incident-face sum at $v$ --- over the parent's annular faces together with the child's --- vanishes mod $3$: \begin{equation} \label{eq:heawood-face-sum-dual} \sum_{f \ni v} \lambda(f) \;\equiv\; 0 \pmod 3 \qquad\text{for every vertex } v \in V(G). \end{equation} Since $\gamma$ carries all faces of $G$ incident to $v$ between the two tires, a family of Heawood face-labellings that is pairwise compatible along every interface of $\mathcal{T}(G, S)$ assembles into a single $\{+1,-1\}$ face-labelling of $G$ satisfying \eqref{eq:heawood-face-sum-dual} at every vertex, hence (by Tait) a proper $4$-vertex-colouring of $G$. \end{remark} \begin{conjecture}[Heawood chain-pigeonhole principle] \label{conj:heawood-chain-pigeonhole} There is a function $N(k)$ such that the following holds. Let \[ T_0 \supset T_1 \supset \cdots \supset T_{N(k)} \] be a nested chain of tires in $\mathcal{T}(G, S)$ whose shared interface cycles have length at most $k$. Then two adjacent Heawood restriction relations $R_{T_i}, R_{T_{i+1}}$ in the chain admit compatible face-labellings along their shared interface (Definition~\ref{def:heawood-compatible}), after rotation and global sign-flip. Equivalently, the chain contains a local gluing step that cannot be obstructed by disjoint Heawood boundary restrictions. \end{conjecture} \begin{conjecture}[Heawood tire route to the Four Colour Theorem] \label{conj:heawood-route-fct} For every plane triangulation $G$ and every level source $S$, the Heawood restriction relations $\{R_T : T \in \mathcal{T}(G, S)\}$ admit a selection of face-labellings that is compatible along every interface of the tire tree. By Remark~\ref{rem:compat-is-heawood} this yields a $\{+1,-1\}$ face-labelling of $G$ satisfying \eqref{eq:heawood-face-sum-dual}, hence $G$ is properly $4$-vertex-colourable. \end{conjecture} %% TODO: realisability of $R_T$ per tire; counting / pigeonhole bound %% giving $N(k)$; orientation/reversal bookkeeping on $\gamma$. \begin{thebibliography}{9} \bibitem{Heawood1898} P.~J.~Heawood, \emph{On the four-colour map theorem}, Quart. J.~Pure Appl. Math. \textbf{29} (1898), 270--285. \bibitem{bauerfeld-depth} E.~Bauerfeld, \emph{Plane Depth}, manuscript (math-research repository), 2026. \bibitem{bauerfeld-nested-tires} E.~Bauerfeld, \emph{Nested Tire Decompositions of Plane Triangulations}, manuscript (math-research repository), 2026. \bibitem{bauerfeld-medial-tires} E.~Bauerfeld, \emph{Medial Tire Decompositions of Plane Triangulations}, manuscript (math-research repository), 2026. \bibitem{bauerfeld-nested-tire-duals} E.~Bauerfeld, \emph{Coloring Nested Tire Dual Graphs}, manuscript (math-research repository), 2026. \end{thebibliography} \end{document}