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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-08-01 11:41:19 +0200 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2024-08-01 11:41:19 +0200 |
commit | c0f6b823fee72db898728ee655235fba0d93644c (patch) | |
tree | f9ca72b8e5ee6ed4ef5cba29a26e83168ec33416 /topology.tex | |
parent | 68184ee466719be94a05a74087bb057aad4f42e8 (diff) | |
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First try at sphere figures.
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-rw-r--r-- | topology.tex | 17 |
1 files changed, 17 insertions, 0 deletions
diff --git a/topology.tex b/topology.tex index 8c21ee9..58e341a 100644 --- a/topology.tex +++ b/topology.tex @@ -139,6 +139,23 @@ $\mathbb M(1)=\frac1N\phi(1)\cdot\mathbf x_0$, the result is \end{aligned} \end{equation} +\begin{figure} + \includegraphics[width=0.49\columnwidth]{figs/connected.pdf} + \hfill + \includegraphics[width=0.49\columnwidth]{figs/shattered.pdf} + + \caption{ + Cartoon of the topology of the CCSP solution manifold implied by our + calculation. The arrow shows the vector $\mathbf x_0$ defining the height + function. The region of solutions is shaded orange, and the critical points + of the height function restricted to this region are marked with a red + point. For $\alpha<1$, there are few simply connected regions with most of + the minima and maxima contributing to the Euler characteristic concentrated + at the height $m_\mathrm a^*$. For $\alpha\geq1$, there are many simply + connected regions and most of their minima and maxima are concentrated at + the equator. + } +\end{figure} \begin{acknowledgements} JK-D is supported by a \textsc{DynSysMath} Specific Initiative of the INFN. |