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\@writefile{toc}{\contentsline {section}{\numberline {2.1}The Valence Quark Structure of the Nucleon}{4}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2.1}{\ignorespaces A measurement of the neutron polarization asymmetry $A_1^n$, determined by the spin structure of the valence quarks made possible by the combination of an 11 GeV beam and the MAD spectrometer in Hall A. The shaded area represents a range of valence quark models; the solid line is a prediction of a pQCD light-cone quark model.}}{5}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2.2}{\ignorespaces A semi-inclusive measurement of $\pi ^+$ and $\pi ^-$ production on the proton and $^3He$ allows a spin and flavor decomposition of the nucleon spin quark distributions. Factorization is assumed but will be tested and quantified by several additional measurements.}}{6}}
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\citation{Sc91}
\citation{Ch78}
\citation{Sc91}
\citation{Ch78}
\@writefile{toc}{\contentsline {subsection}{\numberline {2.2.1}Hadrons in the Nuclear Medium}{14}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2.3}{\ignorespaces  a) $g_2$ spin structure function measured in Hall A using the 11 GeV electron beam and the MAD spectrometer. Neutron $d_2$ matrix element compared to nucleon models and to state of the art Lattice QCD calculations}}{18}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2.4}{\ignorespaces Ratio of the differential $\gamma p \rightarrow \gamma p$ cross section to the Klein-Nishina process on an elementary point-charge $e$, as a function of $s$ at three values of $t$. The ``pQCD'' and ``Handbag'' curves are described in the text. All projected data points are $\pm 5\%$ bins in $t$ and $\pm 2.5\%$ bins in $s$. The data can be obtained at three incident electron energies 6.6, 8.8, and 11.0 GeV, and the configuration described in the Exclusive Reactions section. A total of 1000 production hours is required. }}{19}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2.5}{\ignorespaces  Projected data for the $^3$He form factor $F(Q^2)$ with an 11\nobreakspace  {}GeV JLab beam. Also shown are existing data and predictions of the standard model (IA+MEC)\nobreakspace  {}\cite  {Sc91} and the dimensional-scaling quark model (DSQM)\nobreakspace  {}\cite  {Ch78} }}{20}}
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