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Nathanael A. Fortune edited section_Insert_Theory_Section_HERE__.tex
over 8 years ago
Commit id: 549f47149ff904f47d1f431beb2644f35e50c253
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Contrast two predictions:
\begin{enumerate}
\item in the short mean free path $lambda$ limit, $\Delta E_{\textrm{atom}} = \Delta
E_{\textrm{electron, dip to dip} E_{\textrm{electron}} \textrm{ eV}$
\item in long mean free path $lambda$ limit, $ \Delta E__{\textrm{atom, n}} = E_n - E_{n-1} = [1+ \frac{\lambda}{L} {(2n-1)}]
E_a$ E_a \textrm{ eV}$
\end{enumerate}
where
$E_n$ is the \textit{nth} dip in electron beam current (indicating transfer of energy from electron to atom) and the mean free path depends on the gas density, pressure, and temperature.