\relax 
\citation{charm_DIS}
\citation{charm_jets}
\@writefile{toc}{\contentsline {subsection}{\numberline {0.0.1}Heavy quark production}{1}}
\@writefile{toc}{\contentsline {subsection}{\numberline {0.0.2}Charm production in DIS}{1}}
\@writefile{toc}{\contentsline {subsection}{\numberline {0.0.3}Charm production with jets}{1}}
\citation{beauty}
\@writefile{toc}{\contentsline {subsection}{\numberline {0.0.4}Beauty production}{2}}
\bibcite{charm_DIS}{1}
\bibcite{charm_jets}{2}
\bibcite{beauty}{3}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces The $$\mathop {\mathgroup \symoperators cos}\nolimits \theta ^*$$ distribution in charm-tagged events for $$x_{\gamma }^{\rm  obs}$>0.75$ and $$x_{\gamma }^{\rm  obs}$<0.75$. Predictions from the {\sc  Pythia} MC are compared to the data.}}{5}}
\newlabel{fig:costheta}{{1}{5}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Ratio of low to high $x_{\gamma }^{\rm  obs}$for events with a $D^*$ meson comapred to (a) the SaS1D photon structure functions, (b) the {\sc  Aroma} and {\sc  Cascade} MC models. In (c), the data is extrapolated to the full phase space of the $D^*$ meson and compared to the SaS1D photon structure function.}}{6}}
\newlabel{fig:virt_photon}{{2}{6}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces The transverse momentum of the electron relative to the jet axis, showing the presnece of beauty quarks}}{7}}
\newlabel{fig:b_ptrel}{{3}{7}}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Extrapolated beauty quark cross section compared to NLO QCD predictions}}{8}}
\newlabel{fig:b_nlo}{{4}{8}}