$\begin{figure} \par\includegraphics[width=10.5cm,clip]{0512fig1.eps}\end{figure}$ Figure 1: The lensing geometry. Co-ordinates on the lens plane are denoted with ${\vec x}$ and those on the observer's plane by ${\vec X}$ .
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In the text

$\begin{figure} \par\includegraphics[width=5.8cm,clip]{0512fig2.eps}\end{figure}$ Figure 2: Temporal smearing of a time variable signal (i.e. one for which $\vert\tilde \phi (\nu) \vert(t)$ varies with time) smooths out the variations so that the radiation arrives at the detector over a longer interval and the source potentially falls below the detection threshold.
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In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{0512fig3.eps}\end{figure}$ Figure 3: Diffractive temporal broadening arises because radiation, scattered through a typical angle $\theta _{\rm scat} = (k r_{\rm diff})^{-1}$ , is delayed relative to radiation propagating directly along the line of sight to the source.
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In the text

$\begin{figure} \par\includegraphics[width=7cm,clip]{0512fig4.eps}\end{figure}$ Figure B.1: The geometry showing the distance traversed across the lensing plane in a duration t₀.

In the text

$\begin{figure} \par\includegraphics[width=10.5cm,clip]{0512fig1.eps}\end{figure}$	Figure 1: The lensing geometry. Co-ordinates on the lens plane are denoted with ${\vec x}$ and those on the observer's plane by ${\vec X}$ .
Open with DEXTER

$\begin{figure} \par\includegraphics[width=5.8cm,clip]{0512fig2.eps}\end{figure}$	Figure 2: Temporal smearing of a time variable signal (i.e. one for which $\vert\tilde \phi (\nu) \vert(t)$ varies with time) smooths out the variations so that the radiation arrives at the detector over a longer interval and the source potentially falls below the detection threshold.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{0512fig3.eps}\end{figure}$	Figure 3: Diffractive temporal broadening arises because radiation, scattered through a typical angle $\theta _{\rm scat} = (k r_{\rm diff})^{-1}$ , is delayed relative to radiation propagating directly along the line of sight to the source.
Open with DEXTER