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\@writefile{toc}{\contentsline {section}{Introduction}{1}}
\@writefile{toc}{\contentsline {section}{ Measurements of Non-photonic Electron Production}{1}}
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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces (Color online) The nuclear modification factor, $R_{AA}$, for $d$+Au and Au+Au collisions at $\sqrt  {s_{NN}} = 200$ GeV, together with different theoretical model predictions. Look at Ref. [2] for details.}}{2}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces (Color online) Invariant cross section of electrons from bottom (upper-left) and charm meson (upper-right) decay, together with the ratio of the corresponding measurements to the FONLL predictions for bottom (lower-left) and charm electrons (lower-right), from Ref. \cite  {refc}.}}{3}}
\@writefile{toc}{\contentsline {section}{Direct Reconstruction of Open Charm Mesons }{3}}
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\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces The invariant mass distributions after subtracting backgrounds. $M_{K\pi }$ for $D^0$, $M_{K\pi \pi } - M_{K\pi }$ for $D^{*\pm }$, respectively}}{4}}
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