\subsection{Repeated visits to the small section family} \label{sec:recurrent-axis-sections} We use three copies of the small section, one for each choice of dominant wall. This finite family accommodates the Taub point visited by an orbit without changing the section height or its transverse size along that orbit. For $i=1,2,3$, let $A_i$ be the axis permutation interchanging axis $1$ with axis $i$, with $A_1$ the identity. These are among the six ordered frames and are involutions. Define \begin{equation} \mathcal X_{i,h}(y)=A_i^{-1}\mathcal X_h(y),\qquad E=\mathcal B(d)\cap\mathcal D_h, \qquad \Sigma_{h,d}=\bigcup_{i=1}^3\mathcal X_{i,h}(E), \label{eq:small-axis-section-family} \end{equation} where $\mathcal B(d)$ is~\eqref{eq:whole-small-section}. We retain the label $i$ when using section coordinates, and give the disjoint coordinate space $\{1,2,3\}\times E$ the measure \begin{equation} \mu_{\mathrm{ax}}(H)=\sum_{i=1}^3\mu_h(H_i),\qquad H_i=\{y:(i,y)\in H\}. \label{eq:axis-family-measure} \end{equation} For $d0$, some $t>\max(R,0)$ has \[ \phi_tq=\mathcal X_{i,h}(s,\beta_2,\beta_3),\qquad |s|