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\citation{kicker_proceedings}
\citation{benesch_report}
\@writefile{toc}{\contentsline {section}{\numberline {1}Precision Polarimetry Update}{1}}
\@writefile{toc}{\contentsline {subsection}{\numberline {1.1}M\o ller Polarimeter Operation at High Currents }{1}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces  \em  Polarization measurements using the Hall C M\o ller Polarimeter and a second generation kicker magnet and iron strip target. Globally, the technique yields asymmetries independent of beam current at the several percent level. However, instabilities of unknown origin (likely beam related) make it impossible to show that the kicker system yields measurements stable to 1\%.}}{2}}
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\@writefile{toc}{\contentsline {subsection}{\numberline {1.2}Hall C Compton Polarimeter}{2}}
\citation{MATT}
\citation{coherent_evolution}
\bibcite{kicker_proceedings}{1}
\@writefile{lot}{\contentsline {table}{\numberline {1}{\ignorespaces \em  Operating parameters for a planned beam--kicker system that will allow operation of the Hall C M\o ller Polarimeter at high currents. $\Delta t_{kick}$ refers to the total interval of time for which the beam will be deflected from its nominal path onto a half--foil or strip target. In order to keep beam heating effects to a minimum, the kick interval must be shorter at higher currents.}}{3}}
\newlabel{kicker_op}{{1}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces \em  Schematic of the modifications required to insert the Compton dipole chicane in the Hall C beam line. Additional quadrupoles will be required to achieve a tightly focused beam at the Compton interaction point. The M\o ller Polarimeter will be shifted $\approx $ 11 m closer to the Hall C target position, while other beamline elements, the fast raster for example, will move less by making use of the space between the M\o ller ``vacuum'' legs.}}{4}}
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\bibcite{benesch_report}{2}
\bibcite{MATT}{3}
\bibcite{coherent_evolution}{4}
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