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