source: Backup NB/Talks/NuFact05/NuFact05.aux@ 689

\relax 
\citation{JECACLAL}
\citation{SPL}
\citation{HARP,MINERVA}
\citation{SIMONE1,DONEGA}
\citation{MEZZETTONF02,DONINI04}
\citation{LIPARIxsec}
\citation{GLOBES}
\citation{MEZZETTONF02}
\citation{T2K}
\@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {2}Fluxes}{1}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces The $\nu _\mu $ and the $\mathaccentV {bar}016{\nu }_\mu $ fluxes obtained by optimizing the SPL for a Super Beam case ("SB Opt.") are compared to those obtained with a focusing system designed for a Neutrino Factory ("NF Opt.").}}{1}}
\newlabel{fig:fluxComparison}{{1}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {3}Physics potential}{1}}
\citation{T2K}
\citation{T2K}
\citation{VILLARS}
\bibcite{JECACLAL}{1}
\bibcite{SPL}{2}
\bibcite{HARP}{3}
\bibcite{MINERVA}{4}
\bibcite{SIMONE1}{5}
\bibcite{DONEGA}{6}
\bibcite{MEZZETTONF02}{7}
\bibcite{DONINI04}{8}
\bibcite{LIPARIxsec}{9}
\bibcite{GLOBES}{10}
\bibcite{T2K}{11}
\bibcite{VILLARS}{12}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Comparison of the sensitivity contours with the new optimized setup and the original SPL design after 5 years of running with positive focusing.}}{2}}
\newlabel{fig:SPLDmTheta13Comparison}{{2}{2}}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Comparison of the sensitivity on combined $\theta _{13}$ and $\delta _{CP}$ after 5 years of positive focusing. The T2K sensitivity contour has been derived from reference \cite  {T2K}. No mass hierarchy nor octant hierarchy ambiguity has been considered.}}{2}}
\newlabel{fig:SPLCPSensi}{{3}{2}}