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| 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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