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Cory Balaton
2023-10-24 21:03:15 +02:00
parent 6f34b25e5c
commit 2b83889039
2 changed files with 23 additions and 11 deletions
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latex/sections/results.tex
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@@ -98,7 +98,7 @@ In figure \ref{fig:two_particles_radial_interaction} we see the movement in radi
Finally, by subjecting the system to a time-dependent field, making the replacement in \ref{eq:pertubation}, we study the fraction of particles left at different amplitudes $f$. We can see how the different amplitudes lead to loss of particles, at different angular frequencies $\omega_{V}$ in \ref{fig:wide_sweep}. % Something
When we study ... closer, in figure \ref{fig:} , we observe ... Certain angular frequencies are more effective in pushing particles out of the Penning trap.
When we study the angular frequency $\omega_{V} \in [1.1, 1.7]$ closer, in figure \ref{fig:narrow_sweep}, we observe that there are a few spots where more particles will escape. The most prominent one is where $\omega_V \in [1.1, 1.7]$, and when looking closer to the range, it seems like there's a resonating frequency at around $1.4MHz$ where All the particles will escape no matter the amplitude. When looking at the different angular frequencies with particle interaction like in \ref{fig:narrow_sweep_interactions}, we see that the amount of particles left is roughly the same as when there are no particle interactions, but that it's less predictable.
\begin{figure}[H]
\centering
\includegraphics[width=\linewidth]{images/particles_left_wide_sweep.pdf}
@@ -106,4 +106,16 @@ When we study ... closer, in figure \ref{fig:} , we observe ... Certain angular
\label{fig:wide_sweep}
\end{figure}
\end{document}
\begin{figure}[H]
\centering
\includegraphics[width=\linewidth]{images/particles_left_narrow_sweep.pdf}
\caption{Exploring different angular frequencies more closely}
\label{fig:narrow_sweep}
\end{figure}
\begin{figure}[H]
\centering
\includegraphics[width=\linewidth]{images/particles_left_narrow_sweep_interactions.pdf}
\caption{Exploring particles}
\label{fig:wide_sweep_interactions}
\end{figure}
\end{document}