update: auto commit

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2026-04-09 21:22:10 -04:00
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@@ -321,7 +321,7 @@
\begin{cases} \begin{cases}
\Partial{t}{\phi} = \pi, \\ \Partial{t}{\phi} = \pi, \\
\Partial{t}{\pi} = \tensor{\delta}{^i^j} \Partial{i} \tensor{\psi}{_j},\\ \Partial{t}{\pi} = \tensor{\delta}{^i^j} \Partial{i} \tensor{\psi}{_j},\\
\Partial{t}{\tensor{\psi}{_i}} = \Partial{i} \pi - \gamma \mathcal{C}_i, \Partial{t}{\tensor{\psi}{_i}} = \Partial{i} \pi - \gamma \left( \tensor{\psi}{_i} - \Partial{i} \phi \right),
\end{cases} \end{cases}
\end{equation} \end{equation}
where $\gamma > 0$ is a constant. Then the evolution of the constraints becomes where $\gamma > 0$ is a constant. Then the evolution of the constraints becomes
@@ -331,6 +331,11 @@
which means that the constraint violation will decay exponentially with time, and thus the system is more stable for numerical simulations. which means that the constraint violation will decay exponentially with time, and thus the system is more stable for numerical simulations.
\end{frame} \end{frame}
\begin{frame}{Towards first order Z4c}{constraints during the reduction}
We have to check if the constraint damping term will change the hyperbolicity of the system. The new principal symbol matrix is
\end{frame}
\begin{frame}{Existing first order formulations} \begin{frame}{Existing first order formulations}
\subsection{Existing first order formulations} \subsection{Existing first order formulations}
\begin{itemize} \begin{itemize}