X-Git-Url: https://git.ucc.asn.au/?a=blobdiff_plain;f=thesis%2Fappendices%2Felectron_optics.tex~;h=bfb40e6578f62d0e1091e9139cc1786972e6dc7a;hb=1c9618e52bd8dad6a84c698967800beee8378f24;hp=476baee8d997dc8fc92fd89320d9c13951b71caf;hpb=70a96cca12cb006506461d26cd112bab179fe74c;p=matches%2Fhonours.git

diff --git a/thesis/appendices/electron_optics.tex~ b/thesis/appendices/electron_optics.tex~
index 476baee8..bfb40e65 100644
--- a/thesis/appendices/electron_optics.tex~
+++ b/thesis/appendices/electron_optics.tex~
@@ -1,4 +1,4 @@
-\chapter*{Electron Optics}
+\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 
@@ -44,11 +44,11 @@ The gun was focused using an iterative process, by which each potential was alte
 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.
 
 \begin{center}
-	\includegraphics[scale=0.45, angle=270]{/home/sam/Documents/University/honours/thesis/figures/egun_simulation1.pdf} 
+	\includegraphics[scale=0.45, angle=270]{figures/egun/egun_simulation1.pdf} 
 	
 	\captionof{figure}{{\bf 2D Simulation of trajectories of electrons accelerated through an electron gun}}
 	\label{egun_simulation1.pdf}
-	\includegraphics[scale=0.45, angle=270]{figures/egun_simulation2.pdf} 
+	\includegraphics[scale=0.45, angle=270]{figures/egun/egun_simulation2.pdf} 
 	\captionof{figure}{{\bf 2D Simulation of the electrostatic potential produced by the electron gun}}\label{egun_simulation2.pdf}
 	
 \end{center}