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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces  Photograph of the prototype active collimator installed on top of the total absorption counter in Hall B, as configured for the parasitic beam tests in April 2007. The detector was mounted so that its central hole is at the height of the electron beam while the TAC is in its parked position below the lead brick wall that shields it from the direct photon beam. It was then horizontally scanned across the beam by moving the TAC left and right.}}{2}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces  Current measured on the two inner wedges of the active collimator as it was scanned horizontally through the beam. The green curve is the current measured from the left wedge and the blue from the right. The large inner peaks arise from the beam directly hitting the inner wedges, while the smaller peaks come from the beam interacting in other material and somehow producing current in the inner wedges.}}{3}{}}
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\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces  Current measured on the two outer wedges of the active collimator as it was scanned horizontally through the beam. The green curve is the current measured from the left wedge and the blue from the right. The large outer peaks arise from the beam directly hitting the outer wedges, while the smaller peaks come from the beam interacting in other material and somehow producing current in the inner wedges.}}{4}{}}
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\@writefile{toc}{\contentsline {section}{\numberline {IV}Impact on Primex}{4}{}}
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