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\citation{gaisser}
\@writefile{toc}{\contentsline {section}{\numberline {\uppercase {i}}Introduction}{1}}
\@writefile{toc}{\contentsline {section}{\numberline {\uppercase {ii}}Neutrino beam properties}{1}}
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\@writefile{toc}{\contentsline {subsection}{\numberline {A}Differential spectra}{1}}
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\newlabel{eq1}{{5}{2}}
\newlabel{eq2}{{6}{2}}
\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Calculated neutrino and antineutrino fluxes at a far site located 10000 km from a neutrino factory in which $1 \times 10^{20}$ muons have decayed in the beam--forming straight section. The fluxes are shown as a function of the energy of the stored muons for negative muons (top two plots) and positive muons (bottom two plots), and for three muon polarizations as indicated. FIGURES NEEDS UPDATING}}{2}}
\newlabel{flux_fig}{{1}{3}}
\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Total neutrino flux of a given flavor versus angle at the source from the beamline at $L=732$\nobreakspace  {}km for $E_\mu = 10$\nobreakspace  {}GeV (solid line), 20\nobreakspace  {}GeV (dashed), 50\nobreakspace  {}GeV (dotted), and 250\nobreakspace  {}GeV (dot--dashed), assuming $1.6\times 10^{20}$ neutrinos in the beam per operational year. A Gaussian muon beam divergence of 1\nobreakspace  {}mr has been folded in. The total antineutrino flux is the same. FIGURE NEEDS UPDATING}}{3}}
\newlabel{flux_vs_alpha}{{2}{3}}
\citation{sg_prd}
\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Neutrino and antineutrino spectra for muon--type neutrinos (top) and electron--type neutrinos (bottom) in the beam downstream of a muon storage ring neutrino source containing unpolarized muons. }}{4}}
\newlabel{spectra_fig}{{3}{4}}
\@writefile{toc}{\contentsline {subsection}{\numberline {B}Fluxes}{4}}
\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Distribution of energies for interaction muon--type neutrinos 730\nobreakspace  {}km downstream of the neutrino source for the MINOS PH2 WBB (open histogram) compared with the corresponding distribution downstream of a neutrino factory (shaded histogram).}}{5}}
\newlabel{minos_beam_fig}{{4}{5}}
\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces Energy spectra far cf near from Heidi}}{5}}
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\citation{CCFRtotal, CCFRstrange, Eeightsixtysix}
\@writefile{toc}{\contentsline {subsection}{\numberline {C}Interaction rates}{6}}
\newlabel{exp_a}{{17}{6}}
\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces Lepton energy spectra at a neutrino factory for CC $\overline {\nu }_\mu $ (top left), $\nu _\mu $ (top right), $\nu _e$ (bottom left), and $\overline {\nu }_e$ (bottom right) interactions.}}{7}}
\newlabel{elept_fig}{{6}{7}}
\newlabel{eq8}{{20}{7}}
\newlabel{eq9}{{21}{7}}
\newlabel{eq10}{{22}{7}}
\newlabel{eq11}{{23}{7}}
\newlabel{eq3}{{27}{8}}
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\citation{goodman}
\citation{casper}
\@writefile{lof}{\contentsline {figure}{\numberline {7}{\ignorespaces Tau--neutrino CC cross-section compared with the corresponding muon--neutrino cross-section.}}{9}}
\newlabel{tau_fig}{{7}{9}}
\@writefile{toc}{\contentsline {subsection}{\numberline {D}Beam divergence, momentum spread, and straight-section length}{10}}
\@writefile{lot}{\contentsline {table}{\numberline {\uppercase {i}}{\ignorespaces  Muon neutrino and electron antineutrino CC interaction rates in the absence of oscillations, calculated for baseline length $L = 732$\nobreakspace  {}km (FNAL $\rightarrow $ Soudan), for MINOS using the wide band beam and a muon storage ring with $E_\mu =10, 20, 50$ and $250$\nobreakspace  {}GeV. }}{10}}
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\newlabel{rates_tab}{{\uppercase {i}}{10}}
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\bibcite{lipari2}{27}
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\bibcite{cern_vision}{40}
\bibcite{gaisser}{41}
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\bibcite{casper}{44}
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\bibcite{bpw80}{48}
\bibcite{kuo}{49}
\bibcite{totsuka}{50}
\bibcite{earth}{51}
\bibcite{parke}{52}
\bibcite{lipari}{53}
\bibcite{petcov}{54}
\bibcite{other_matter}{55}
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\bibcite{pantaleone}{57}
\bibcite{bdppw}{58}
\bibcite{hall}{59}
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