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author | Urbain Vaes <urbain@vaes.uk> | 2023-09-16 19:00:39 +0200 |
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committer | Urbain Vaes <urbain@vaes.uk> | 2023-09-16 19:00:39 +0200 |
commit | e64a03583d84c663f302e53886783179496ae517 (patch) | |
tree | 70da87cea6cf1fac84d4f411b247790e6a5d4a21 /main.tex | |
parent | 2a18bd93c8022a193dcc4d7e0569d9cde3bcf228 (diff) |
Add slide
Diffstat (limited to 'main.tex')
-rwxr-xr-x | main.tex | 13 |
1 files changed, 13 insertions, 0 deletions
@@ -58,6 +58,7 @@ \begin{frame} {Some references} \begin{itemize} + \itemsep.2cm \item \fullcite{MR3509213} \item \fullcite{pavliotis2011applied} \item Lecture notes by Gabriel Stoltz on computational statistical physics: @@ -108,6 +109,7 @@ \[ \rho = \int_{0}^{\infty} \expect_{\mu} \bigl[\varphi(x_t) \phi(x_0)\bigr] \, \d t. \] + We will derive this formula from linear response. \item Transient techniques: \end{itemize} @@ -136,6 +138,17 @@ \end{theorem} \end{frame} +\begin{frame} + {Existence of an invariant measure for noneq.\ dynamics} + Consider the paradigmatic dynamics + \begin{align*} + \d q_t &= M^{-1} p_t \, \d t, \\ + \d p_t &= - \bigl(\grad V(q_t) + \eta F\bigr) \, \d t - \gamma M^{-1} p_t \, \d t + \sqrt{\frac{2 \gamma}{\beta}} \, \d W_t, + \end{align*} + where $(q_t, p_t) = \torus^d \times \real^d$ and $F \in \real^d$ with $\abs{F} = 1$ is a given direction. + +\end{frame} + \end{document} % vim: ts=2 sw=2 |