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\citation{lawrence1}
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\citation{lawrence2}
\citation{dzierba}
\citation{semenov1}
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\citation{semenov2}
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\citation{kloe}
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\@writefile{toc}{\contentsline {section}{\numberline {4}The KLOE Experience}{5}}
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\@writefile{toc}{\contentsline {section}{\numberline {5}Margins/Contingency}{5}}
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\bibcite{kloe}{6}
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\citation{lawrence2}
\citation{dzierba}
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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces  This figure shows the percent improvement in the average time and time difference resolution of the {\sc  BCAL}\ in going from the 3-3-4 to the 1-2-3-4 segmentation\nobreakspace  {}\cite  {lawrence2}. The simulation at 90$^\circ $ shows that the two segmentations offer similar resolution; these points were not shown for ease of scaling the graph. As noted above, the region below 30$^\circ $ is vital for the investigation of exotics. }}{7}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces  This scatterplot\nobreakspace  {}\cite  {dzierba} shows the energy versus angle for the lowest energy photon in the event for $\gamma p \rightarrow b_1 \pi ^0 n$. The region below 30$^\circ $ is vital for the investigation of exotics, and here the energies of the photon span a great range. This scatterplot demonstrates the challenge for this lowest energy photon reconstruction: a large number of the low energy photons occur near the edge of the {\sc  BCAL}. }}{7}}
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\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces  These plots show the the suppression of neutrons for a fixed angle (20$^\circ $). This was calculated from a probability hypothesis, which is based on mono-energetic photons and all neutrons that deposit the same energy in the entire module. Two energies were studied, 0.45\nobreakspace  {}GeV and 1\nobreakspace  {}GeV. Note that two segmentations are equivalent in the 90\%-100\% photon efficiency range, but diverge quickly below that. The gain in going to the 1-2-3-4 segmentation is evident in comparing the neutron efficiencies, for data subsets, e.g. in the 50-90\% efficiency range. Such subsets are very useful in tuning the analysis code and establishing the confidence in exotic extraction. }}{8}}
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\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces  We have studied the identification of pions and protons from the reaction $\gamma p \rightarrow \pi _1(1600) \mskip \medmuskip  n \rightarrow b_1 \pi ^+ p$, with secondary decay products. The particle identification for protons and pions is shown for the 1-2-3-4 segmentation in the top panel; the 3-3-4 segmentation looks qualitatively similar. Projected slices in momentum from both plots were taken and fitted, as shown in the left panel of the bottom row. A comparison of these fits is shown in the bottom-right plot, demonstrating that the $\pi ^+ \delta \beta $ resolution improves by about 18\% in the momentum region where the bands of the protons and positive pions begin to merge. Ê In the simulation it was assumed that the charged-particle timing resolution improvement for the 1-2-3-4 segmentation is identical to that of photon clusters. No background events were included.}}{9}}
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\@writefile{lot}{\contentsline {table}{\numberline {1}{\ignorespaces  This table shows the cost to instrument the innermost ring of the {\sc  BCAL}.}}{10}}
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