\relax 
\@writefile{lot}{\contentsline {table}{\numberline {1}{\ignorespaces Operating parameters for an experiment}}{2}}
\newlabel{cdr_rates}{{1}{2}}
\@writefile{lot}{\contentsline {table}{\numberline {2}{\ignorespaces Dependence of source parameters on electron beam energy}}{3}}
\newlabel{new_rates}{{2}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces  Degree of linear polarization {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 10 GeV electron beam, with collimation (solid curve) and without (dashed curve).}}{4}}
\newlabel{polar10}{{1}{4}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces  Degree of linear polarization {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 11 GeV electron beam, with collimation (solid curve) and without (dashed curve).}}{5}}
\newlabel{polar11}{{2}{5}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces  Degree of linear polarization {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 12 GeV electron beam, with collimation (solid curve) and without (dashed curve).}}{6}}
\newlabel{polar12}{{3}{6}}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces  Degree of linear polarization {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 13 GeV electron beam, with collimation (solid curve) and without (dashed curve).}}{7}}
\newlabel{polar13}{{4}{7}}
\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces  Photon beam rates {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 10 GeV electron beam, with collimation (solid curve) and without (dashed curve). Rates are normalized as shown in Table\nobreakspace  {}2\hbox {}.}}{8}}
\newlabel{flux10}{{5}{8}}
\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces  Photon beam rates {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 11 GeV electron beam, with collimation (solid curve) and without (dashed curve). Rates are normalized as shown in Table\nobreakspace  {}2\hbox {}.}}{9}}
\newlabel{flux11}{{6}{9}}
\@writefile{lof}{\contentsline {figure}{\numberline {7}{\ignorespaces  Photon beam rates {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 12 GeV electron beam, with collimation (solid curve) and without (dashed curve). Rates are normalized as shown in Table\nobreakspace  {}2\hbox {}.}}{10}}
\newlabel{flux12}{{7}{10}}
\@writefile{lof}{\contentsline {figure}{\numberline {8}{\ignorespaces  Photon beam rates {\it  vs} photon energy for the GlueX coherent bremsstrahlung source for a 13 GeV electron beam, with collimation (solid curve) and without (dashed curve). Rates are normalized as shown in Table\nobreakspace  {}2\hbox {}.}}{11}}
\newlabel{flux13}{{8}{11}}
\@writefile{lof}{\contentsline {figure}{\numberline {9}{\ignorespaces  Photon beam figure of merit, defined by Eq.\nobreakspace  {}1\hbox {}, plotted as a function of the radiator-collimator distance, for a variety of collimator apertures (colored curves) and for no collimator (black curve). The vertical scale is defined by setting the FOM for the uncollimated case to unity.}}{12}}
\newlabel{fomvsD}{{9}{12}}
\@writefile{lof}{\contentsline {figure}{\numberline {10}{\ignorespaces  Photon beam figure of merit, defined by Eq.\nobreakspace  {}1\hbox {}, plotted as a function of the electron beam energy, under conditions of constant total hadronic background rates in the detector. The green curve is for a 3.4 mm collimator at 80 m from the radiator, and the black curve is for an uncollimated beam.}}{13}}
\newlabel{fomvsE}{{10}{13}}
\newlabel{fom}{{1}{14}}