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\citation{lawson}
\citation{Pantel}
\citation{rodionEPAC}
\citation{xievac}
\citation{rodionEPAC}
\@writefile{toc}{\contentsline {section}{\uppercase {Introduction}}{1}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces The laser beam comes from left. After propagating passing through a lens (L1) and bouncing on an apertured mirror (M1), the beam co-propagates with the e$^-$ beam through the open iris-loaded structure [(OILS) green rectangle]. The laser beam is then extracted from the chamber thanks to a second aperture mirror (M2) and then transported to a diagnostics station.}}{1}}
\newlabel{fig:over}{{1}{1}}
\@writefile{toc}{\contentsline {section}{\uppercase {The open iris-loaded structure concept}}{1}}
\newlabel{eq:lsr}{{1}{1}}
\@writefile{toc}{\contentsline {section}{\uppercase {Generation of TM$_{01}^*$ mode}}{1}}
\citation{piotfnpl}
\citation{gfel1}
\citation{gfel1}
\citation{astra}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces  Measured transverse density {\bf  a)} and corresponding line profile {\bf  b)} of the TM$_{01}^*$ mode. }}{2}}
\newlabel{fig:Resultdonuts}{{2}{2}}
\newlabel{fig:Resultdonuts}{{2}{2}}
\@writefile{lot}{\contentsline {table}{\numberline {1}{\ignorespaces FNPL nominal operating settings and simulated parameters for 100\nobreakspace  {}pC bunch.}}{2}}
\newlabel{tab:fnpl}{{1}{2}}
\@writefile{toc}{\contentsline {section}{\uppercase {expected performances at FNPL}}{2}}
\newlabel{eqn:index}{{3}{2}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Sensitivity of energy gain on gas pressure (a) and required gas pressure for incoming energy (b)\nobreakspace  {}.}}{2}}
\newlabel{fig:pressure}{{3}{2}}
\citation{piotfnpl}
\bibcite{lawson}{1}
\bibcite{Pantel}{2}
\bibcite{rodionEPAC}{3}
\bibcite{xievac}{4}
\bibcite{astra}{5}
\bibcite{gfel1}{6}
\bibcite{piotfnpl}{7}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces longitudinal phase space (top) upstream (input), and at different locations downstream of the OILS section entrance (5, 10 and 20\nobreakspace  {}cm) along with the associated charge density (bottom) ($s>0$ corresponds to the bunch head).}}{3}}
\newlabel{fig:mubunching}{{4}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces Sensitivity of the energy spectrum on the incoming e$^-$ beam energy spread ($\sigma _{x,y}=0.1$\nobreakspace  {}mm). }}{3}}
\newlabel{fig:dpp}{{5}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces Simulated energy spectrum for various e$^-1$ beam sizes in the OILS structure (left) and corresponding energy spread (right). Note for $\sigma _{x,y}>0.2$\nobreakspace  {}mm, the beam is not fully transmitted ($\sigma _{E}=10$\nobreakspace  {}keV). (Note: the profile corresponding to the ``laser off" case has been scaled by 1/10.) }}{3}}
\newlabel{fig:param}{{6}{3}}
\@writefile{toc}{\contentsline {section}{\uppercase {Conclusion}}{3}}
\@writefile{toc}{\contentsline {section}{\uppercase {REFERENCES}}{3}}
