-\appendix{Electron Optics}
-
-
-There are two goals of electron optics as applied to total current spectroscopy (and other forms of electron scattering experiments): firstly, to produce the narrowest possible distribution $f(E - E_1)$ of primary electron energies at the sample, and secondly, to ensure that
+\section{Electron Optics}
The electron gun used for this study contains a total of ten electrodes, with six independently adjustable groups. Figure \ref{egun_simulation1.pdf} illustrates a cross section of the gun, using colour coding to indicate groups of electrodes which are kept at the same potential.
The first electrode, which houses the cathode, providing a narrow apparture for electrons to exit. A positive potential (of the order of $10V$ applied to the Wenhalt causes electrons leaving the cathode to be accelerated into a narrow beam.
- It is difficult to control the focusing properties of the gun using the Wenhalt alone; the main purpose of the Wenhalt is to create a high current, narrow beam of electrons, which can be focused by the other electrodes in the gun. If the potential applied to the Wenhalt is too high, electrons will be drawn into its surface. If the Wenhalt potential is too low, then the
+ It is difficult to control the focusing properties of the gun using the Wenhalt alone; the main purpose of the Wenhalt is to create a high current, narrow beam of electrons, which can be focused by the other electrodes in the gun. If the potential applied to the Wenhalt is too high, electrons will be drawn into its surface. If the Wenhalt potential is too low, then fewer electrons are able to leave the aparture.
\item {\bf Einzel Lens }
\item {\bf Final Electrode}
- The electron gun was originally designed for use in a Cathode Ray Oscilloscope (CRO). This electrode is held just in front of a flurescent screen, but is not electrically connected to the screen. When accellerated electrons strike the screen, they are
+ The electron gun was originally designed for use in a Cathode Ray Oscilloscope (CRO). This electrode is held just in front of a flurescent screen, but is not electrically connected to the screen. The final electrode is held at the same potential as the accelerating electrodes in the Einzel lens.
In the total current spectroscopy experiments, this electrode is typically at a much higher potential than the surface under bombardment. As a result, low energy primary electrons may be deflected or even turned back towards the gun, rather than striking the surface. This effect can be exploited to narrow the energy distribution of primary electrons at the surface, but also has the effect of greatly reducing the current of primary electrons reaching the surface.
\end{enumerate}
In preparation for Total Current Spectroscopy experiments, the effect of each of the controllable potentials was investigated by focusing the electron gun on its original flurescent screen. However, when repurposed for total current spectroscopy, the gun needed to be refocused several times (with changing sample holder design).
-From \ref{tcs_theory1}, it is apparent that the electron gun should be focused to achieve the maximum possible resolution by producing the narrowest possible primary energy distribution at the target. In addition, to increase the energy range (relative to the target), it
-
The gun was focused using an iterative process, by which each potential was altered in turn to maximise the current.
\pagebreak
-\section{A two dimensional electron gun simulation}
+\subsection{A two dimensional electron gun simulation}
The below figures \ref{egun_simulation1.pdf} and \ref{egun_simulation2.pdf} are the results of a simplistic electron gun simulation. The results of this simulation were not used to focus the actual electron gun; the images shown here are purely presented as a visual aid.
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