| Rev | Line | |
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| [400] | 1 | \relax
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| 2 | \citation{JECACLAL}
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| 3 | \citation{SPL}
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| 4 | \citation{HARP,MINERVA}
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| 5 | \citation{SIMONE1,DONEGA}
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| 6 | \citation{MEZZETTONF02,DONINI04}
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| 7 | \citation{LIPARIxsec}
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| 8 | \citation{GLOBES}
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| 9 | \citation{MEZZETTONF02}
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| 10 | \citation{T2K}
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| 11 | \@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}}
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| 12 | \@writefile{toc}{\contentsline {section}{\numberline {2}Fluxes}{1}}
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| 13 | \@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}}
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| 14 | \newlabel{fig:fluxComparison}{{1}{1}}
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| 15 | \@writefile{toc}{\contentsline {section}{\numberline {3}Physics potential}{1}}
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| 16 | \citation{T2K}
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| 17 | \citation{T2K}
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| 18 | \citation{VILLARS}
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| 19 | \bibcite{JECACLAL}{1}
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| 20 | \bibcite{SPL}{2}
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| 21 | \bibcite{HARP}{3}
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| 22 | \bibcite{MINERVA}{4}
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| 23 | \bibcite{SIMONE1}{5}
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| 24 | \bibcite{DONEGA}{6}
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| 25 | \bibcite{MEZZETTONF02}{7}
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| 26 | \bibcite{DONINI04}{8}
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| 27 | \bibcite{LIPARIxsec}{9}
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| 28 | \bibcite{GLOBES}{10}
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| 29 | \bibcite{T2K}{11}
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| 30 | \bibcite{VILLARS}{12}
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| 31 | \@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}}
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| 32 | \newlabel{fig:SPLDmTheta13Comparison}{{2}{2}}
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| 33 | \@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}}
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| 34 | \newlabel{fig:SPLCPSensi}{{3}{2}}
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