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\emailauthor{somov@jlab.org}{A.Somov\corref {cor1}}
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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Schematic layout of the GlueX detector (not to scale). Numbers represent the following detector components: Solenoid magnet (1), barrel calorimenter (2), central drift chambers (3), forward drift chambers (4), time-of-flight wall(5).}}{2}}
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\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces The ratio of LED to $\alpha $-source signals for different run periods.}}{4}}
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\@writefile{lof}{\contentsline {figure}{\numberline {10}{\ignorespaces Energy resolution measured in the 3x3 cell region as a function of the photon energy.}}{5}}
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\@writefile{lof}{\contentsline {figure}{\numberline {11}{\ignorespaces Rates of the CCAL modules during PrimEx $\eta $ production run. The energy threshold corresponds to 30 MeV.}}{6}}
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\@writefile{lof}{\contentsline {figure}{\numberline {12}{\ignorespaces Elasticity distribution of reconstructed Compton candidates.}}{7}}
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\@writefile{lof}{\contentsline {figure}{\numberline {13}{\ignorespaces FCAL frame with calorimeter modules installed: $PbWO_{\rm  4}$ 4 crystals (brown area), lead glass blocks (green).}}{7}}
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\@writefile{lof}{\contentsline {figure}{\numberline {14}{\ignorespaces Magnetic field distribution inside the shield housing as a function of the distance from the housing face. Plot (a) corresponds to the longitudinal field and plot (b) corresponds to the transverse field. Markers denote different fields produced by Helmholtz coils. }}{7}}
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\@writefile{lof}{\contentsline {figure}{\numberline {15}{\ignorespaces  Signal amplitudes of shielded PMT induced by an LED as a function of the magnetic field (a). Amplitudes, normalized to measurements without magnetic field (b). PMT response was measured for different intensities of light pulse and HV settings as shown by different polymarkers.}}{7}}
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