[387] | 1 | % |
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| 2 | % bibtex is used for bibliography |
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| 3 | % - put your references in file Frejus.bib, in bibtex format |
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| 4 | % (you can get it directly from spires). |
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| 5 | % No need to worry about the order of citation |
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| 6 | % - to process file, do |
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| 7 | % latex Frejus |
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| 8 | % bibtex Frejus |
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| 9 | % latex Frejus |
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| 10 | % |
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| 11 | %\documentstyle[12pt,epsfig,amstex,amssymb,here]{article} |
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| 12 | \documentclass[12pt]{article} |
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| 13 | \usepackage{epsfig,amsmath,amssymb,here,rotating} |
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| 14 | \usepackage[T1]{fontenc} |
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| 15 | \usepackage{eurosym} |
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| 16 | %\usepackage{eurosans} |
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| 17 | \newcommand{\modif}[3]{{(\sc{#1})}{\sout{\small #2}}{\bf #3}} |
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| 18 | |
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| 19 | % |
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| 20 | |
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| 21 | \def\dm{\ensuremath{\Delta m}} |
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| 22 | \def\dm2{\ensuremath{\Delta m^{2}\ }} |
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| 23 | \def\sen2th{\ensuremath{ \sin^{2}(2\theta)\ }} |
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| 24 | \def\(({\left(} |
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| 25 | \def\)){\right)} |
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| 26 | |
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| 27 | \def\nubar{$\overline{\nu}\ $} |
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| 28 | \def\nue{\ensuremath{\nu_{e}\ }} |
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| 29 | \def\nubare{\ensuremath{\overline{\nu}_{e}\ }} |
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| 30 | \def\nubarecc{$\overline{\nu}_{e}^{CC}\ $} |
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| 31 | \def\numu{\ensuremath{\nu_{\mu}\ }} |
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| 32 | \def\nubarmu{\ensuremath{\overline{\nu}_{\mu}\ }} |
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| 33 | \def\nubarmucc{$\overline{\nu}_{\mu}^{CC}\ $} |
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| 34 | \def\nutau{\ensuremath{\nu_{\tau}\ }} |
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| 35 | \def\nubartau{\ensuremath{\overline{\nu_{\tau}}\ }} |
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| 36 | \def\nulep{$\nu^{l}\ $} |
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| 37 | \def\nubarlep{$\overline{\nu^{l}}\ $} |
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| 38 | |
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| 39 | \def\nuef{\ensuremath{\nu_{e}}} |
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| 40 | \def\nubarf{\ensuremath{\overline{\nu}}} |
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| 41 | \def\nubaref{\ensuremath{\overline{\nu}_{e}}} |
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| 42 | \def\numuf{\ensuremath{\nu_{\mu}}} |
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| 43 | \def\nubarmuf{\ensuremath{\overline{\nu_{\mu}}}} |
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| 44 | \def\nutauf{\ensuremath{\nu_{\tau}}} |
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| 45 | \def\nubartauf{\ensuremath{\overline{\nu_{\tau}}}} |
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| 46 | \def\nulepf{\ensuremath{\nu^{l}}} |
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| 47 | \def\nubarlepf{\ensuremath{\overline{\nu^{l}}}} |
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| 48 | \def\pzero{\ensuremath{\ensuremath{\pi^0\ }}} |
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| 49 | |
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| 50 | %\newcommand{\pion}{\ensuremath{\pi}} |
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| 51 | %\newcommand{\pinot}{\ensuremath{\pi^0}} |
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| 52 | %\newcommand{\phad}{\ensuremath{\vec{p}_{had}}} |
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| 53 | \newcommand{\mphad}{\ensuremath{p_{had}}} |
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| 54 | \newcommand{\plep}{\ensuremath{\vec{p}_{lep}}} |
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| 55 | \newcommand{\pele}{\ensuremath{\vec{p}_{ele}}} |
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| 56 | \newcommand{\mpele}{\ensuremath{p_{lep}}} |
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| 57 | \newcommand{\evis}{\ensuremath{E_{vis}\,}} |
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| 58 | \newcommand{\pte}{\ensuremath{p^T_e}} |
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| 59 | \newcommand{\ptlep}{\ensuremath{p^T_{lepton}}} |
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| 60 | \newcommand{\nuecc}{\ensuremath{\nu_e^{CC}\,}} |
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| 61 | \newcommand{\numucc}{\ensuremath{\nu_\mu^{CC}\,}} |
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| 62 | \newcommand{\numunc}{\ensuremath{\nu_\mu^{NC}}} |
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| 63 | \newcommand{\antinuecc}{\ensuremath{\overline{\nu_e}^{CC}\,}} |
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| 64 | \newcommand{\antinumucc}{\ensuremath{\overline{\nu_\mu}^{CC}}} |
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| 65 | |
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| 66 | \newcommand{\chisq}{\ensuremath{\chi^{2}\ }} |
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| 67 | |
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| 68 | \newcommand{\raw}{\rightarrow} |
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| 69 | \newcommand{\nn}{\nonumber} |
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| 70 | % |
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| 71 | \newcommand{\ev}{ {\rm eV} } |
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| 72 | \newcommand{\gev}{ {\rm GeV} } |
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| 73 | \newcommand{\Gev}{ {\rm GeV} } |
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| 74 | \newcommand{\tev}{ {\rm TeV} } |
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| 75 | \newcommand{\mev}{ {\rm MeV} } |
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| 76 | \newcommand{\Mev}{ {\rm MeV} } |
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| 77 | \newcommand{\mw}{ {\rm MW} } |
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| 78 | \newcommand{\km}{ {\rm km} } |
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| 79 | \newcommand{\tesla}{ {\rm Tesla} } |
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| 80 | \newcommand{\meter}{ {\rm m} } |
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| 81 | \newcommand{\kton}{ {\rm Kton} } |
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| 82 | \newcommand{\ton}{ {\rm ton} } |
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| 83 | \newcommand{\mton}{ {\rm Mton} } |
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| 84 | \newcommand{\mm}{ {\rm mm} } |
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| 85 | \newcommand{\cm}{ {\rm cm} } |
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| 86 | \newcommand{\mim}{ {\mu \rm m} } |
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| 87 | %\newcommand{\bea}{\begin{eqnarray}} |
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| 88 | %\newcommand{\eea}{\end{eqnarray}} |
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| 89 | \newcommand{\be}{\begin{equation}} |
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| 90 | \newcommand{\ee}{\end{equation}} |
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| 91 | % |
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| 92 | \newcommand{\flux}{\mbox{$ cm^{-2}~s^{-1}$}} |
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| 93 | \newcommand{\dens}{\mbox{$ cm^{-3}$}} |
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| 94 | % |
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| 95 | \newcommand{\tetaot}{\mbox{$\theta_{13}$}} |
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| 96 | \newcommand{\tetatt}{\mbox{$\theta_{23}$}} |
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| 97 | \newcommand{\tatm}{\mbox{$\theta_{23}$}} |
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| 98 | \newcommand{\tsun}{\mbox{$\theta_{12}$}} |
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| 99 | \newcommand{\deltt}{\mbox{$\Delta_{23}$}} |
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| 100 | \newcommand{\delot}{\mbox{$\Delta_{13}$}} |
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| 101 | \newcommand{\dsun}{\mbox{$\Delta_{sun}^2$}} |
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| 102 | \newcommand{\datm}{\mbox{$\Delta_{atm}^2$}} |
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| 103 | |
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| 104 | % |
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| 105 | \newcommand{\Losc}{\mbox{$L_{osc}$}} |
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| 106 | \newcommand{\mmm}{\mbox{$m_{1}^{2}-m_{2}^{2}$}} |
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| 107 | \newcommand{\stt}{\mbox{$sin^{2}~2\theta $}} |
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| 108 | \newcommand{\dms}{\mbox{$\Delta m^{2}$}} |
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| 109 | \newcommand{\numubar}{\mbox{$\overline{\nu}_{\mu}$}} |
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| 110 | \newcommand{\nuebar}{\mbox{$\overline{\nu}_{e}$}} |
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| 111 | \newcommand{\muminus}{\mbox{$\mu^{-}$}} |
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| 112 | \newcommand{\muplus}{\mbox{$\mu^{+}$}} |
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| 113 | |
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| 114 | \newcommand{\neb}{\mbox{$\overline{\nu}_{e}$}} |
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| 115 | \newcommand{\num}{\mbox{${\nu}_{\mu}$}} |
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| 116 | \newcommand{\nmb}{\mbox{$\overline{\nu}_{\mu}$}} |
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| 117 | \newcommand{\nut}{\mbox{${\nu}_{\tau}$}} |
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| 118 | \newcommand{\ntb}{\mbox{$\overline{\nu}_{\tau}$}} |
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| 119 | \newcommand{\nub}{\mbox{$\overline{\nu}$}} |
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| 120 | \newcommand{\lsim}{\mbox{\raisebox{-1.ex} |
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| 121 | {$\stackrel{\textstyle <}{\textstyle \sim}$}}} |
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| 122 | \newcommand{\gsim}{\mbox{\raisebox{-1.ex} |
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| 123 | {$\stackrel{\textstyle >}{\textstyle \sim}$}}} |
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| 124 | \newcommand{\sstt} {\sin^2 2\theta} |
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| 125 | %\newcommand{\dms} {\Delta m^2} |
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| 126 | \newcommand{\degree} {^{\circ}} |
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| 127 | |
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| 128 | \newcommand{\ttbs}{\char'134} |
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| 129 | %\newcommand{\AmS}{{\protect\the\textfont2 A\kern-.1667em\lower.5ex\hbox{M}\kern-.125emS}} |
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| 130 | |
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| 131 | \newcommand{\pnuenumu}{\ensuremath{P(\nue \rightarrow \numu)\,}} |
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| 132 | %\newcommand{\pnumunumu}{\ensuremath{p(\numu \rightarrow \numu)\,}} |
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| 133 | \newcommand{\nuenumu}{\ensuremath{\nue \rightarrow \numu\,}} |
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| 134 | \newcommand{\numunutau}{\ensuremath{\numu \rightarrow \nutau\,}} |
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| 135 | \newcommand{\nuenutau}{\ensuremath{\nue \rightarrow \nutau}} |
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| 136 | \newcommand{\nubarenubarmu}{\ensuremath{\overline{\nu}_e \rightarrow \overline{\nu}_\mu\,}} |
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| 137 | \newcommand{\nubarmunubare}{\ensuremath{\overline{\nu}_\mu \rightarrow \overline{\nu}_e\,}} |
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| 138 | \newcommand{\dmot}{\ensuremath{\Delta m^2_{12}\,}} |
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| 139 | \newcommand{\dmtt}{\ensuremath{\Delta m^2_{23} \,}} |
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| 140 | |
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| 141 | \newcommand{\He}{\ensuremath{^6{\mathrm{He}\,}}} |
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| 142 | \newcommand{\Ne}{\ensuremath{^{18}{\mathrm{Ne}\,}}} |
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| 143 | \def\Li{^6{\mathrm{Li}}} |
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| 144 | \def\anue{\overline{{\mathrm\nu}}_{\mathrm e}} |
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| 145 | \def\anumu{\overline{{\mathrm\nu}}_{\mathrm \mu}} |
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| 146 | \newcommand{\thetaot}{\ensuremath{\theta_{13}}\,} |
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| 147 | \newcommand{\thetatt}{\ensuremath{\theta_{23}}\,} |
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| 148 | \newcommand{\numunue}{\ensuremath{\nu_\mu \rightarrow \nu_e}} |
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| 149 | \newcommand{\pnuenue}{\ensuremath{P(\nue \rightarrow \nue)}} |
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| 150 | \newcommand{\pnumunue}{\ensuremath{P(\nu_\mu \rightarrow \nu_e)}} |
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| 151 | \newcommand{\pnumunumu}{\ensuremath{P(\nu_\mu \rightarrow \nu_\mu)}} |
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| 152 | \newcommand{\pnubarenubarmu}{\ensuremath{P(\overline{\nu}_e \rightarrow \overline{\nu}_\mu\)\,}} |
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| 153 | \newcommand{\pnubarmunubare}{\ensuremath{P(\overline{\nu}_\mu \rightarrow \overline{\nu}_e)\,}} |
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| 154 | \newcommand{\dmsun}{\ensuremath{\Delta m^2_{sun}\ }} |
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| 155 | \newcommand{\dmatm}{\ensuremath{\Delta m^2_{atm}}} |
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| 156 | \newcommand{\nueovernumu}{\ensuremath{\nue/\numu}} |
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| 157 | \newcommand{\sigdm}{\ensuremath{{\rm sign}(\Delta m^2_{23})\ }} |
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| 158 | %\newcommand{\delCP}{\ensuremath{\delta_{\rm CP}}} |
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| 159 | \newcommand{\delCP}{\ensuremath{\delta_{\rm CP}\ }} |
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| 160 | |
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| 161 | \newcommand{\stheta}{\sin^22\theta_{13}} |
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| 162 | \newcommand{\deltacp}{\delta_\mathrm{CP}} |
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| 163 | |
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| 164 | \def\He{\ensuremath{^6{\mathrm{He}}}} |
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| 165 | \def\Li{\ensuremath{^6{\mathrm{Li}}}} |
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| 166 | \def\Ne{\ensuremath{^{18}{\mathrm{Ne}}}} |
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| 167 | \def\anue{\ensuremath{\overline{{\mathrm\nu}}_{\mathrm e}}} |
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| 168 | \def\anumu{\ensuremath{\overline{{\mathrm\nu}}_{\mathrm \mu}}} |
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| 169 | \def\numunue{\ensuremath{\mbox{$\nu_\mu \rightarrow \nu e$}}} |
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| 170 | |
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| 171 | % |
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| 172 | % |
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| 173 | \newcommand{\REDBLA}[1]{\red {#1} \black} |
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| 174 | % |
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| 175 | \def\mc2{\multicolumn{2}{c|}} |
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| 176 | % |
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| 177 | %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% |
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| 178 | |
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| 179 | \input{style.tex} |
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| 180 | |
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| 181 | \begin{document} |
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| 182 | |
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| 183 | \bibliographystyle{JHEP} |
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| 184 | |
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| 185 | \begin{titlepage} |
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| 186 | |
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| 187 | %\vspace*{2cm} |
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| 188 | |
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| 189 | \begin{center} |
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| 190 | {\bf \Large MEMPHYS\,:} |
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| 191 | |
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| 192 | \vspace{0.2cm} |
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| 193 | |
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| 194 | {\bf \Large A large scale water \v{C}erenkov detector at Fr\'ejus} |
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| 195 | |
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| 196 | %\vspace{0.5cm} |
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| 197 | %{\bf Preliminary } |
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| 198 | |
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| 199 | %\vspace{1.5cm} |
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| 200 | %{\bf Contribution to the CERN strategic committee} \\ |
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| 201 | %Orsay, 30/01/2006 |
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| 202 | \end{center} |
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| 203 | |
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| 204 | \vspace{2.5cm} |
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| 205 | |
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| 206 | \begin{center} |
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| 207 | |
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| 208 | {A. de Bellefon$^{(1)}$, |
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| 209 | J. Bouchez$^{(1)}$$^{(2)}$, |
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| 210 | J. Busto$^{(3)}$, |
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| 211 | J.-E. Campagne$^{(4)}$, \\ |
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| 212 | C. Cavata$^{(2)}$, %S. Davidson$^{(5)}$, |
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| 213 | J. Dolbeau$^{(1)}$, |
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| 214 | J. Dumarchez$^{(5)}$, |
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| 215 | P. Gorodetzky$^{(1)}$, |
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| 216 | S. Katsanevas$^{(1)}$, \\ |
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| 217 | M. Mezzetto$^{(6)}$, |
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| 218 | L. Mosca$^{(2)}$, |
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| 219 | T. Patzak$^{(1)}$, % Joel Pouthas$^{(7)}$, |
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| 220 | P. Salin$^{(1)}$, |
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| 221 | A. Tonazzo$^{(1)}$, |
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| 222 | C. Volpe$^{(7)}$} |
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| 223 | |
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| 224 | \vspace{0.5cm} |
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| 225 | {\it $^{(1)}$ APC Paris \\ |
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| 226 | $^{(2)}$ DAPNIA-CEA Saclay \\ |
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| 227 | $^{(3)}$ CPP Marseille \\ |
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| 228 | $^{(4)}$ LAL Orsay \\ |
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| 229 | % $^{()}$ IPN Lyon \\ |
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| 230 | $^{(5)}$ LPNHE Paris \\ |
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| 231 | $^{(6)}$ INFN Padova \\ |
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| 232 | $^{(7)}$ IPN Orsay |
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| 233 | } |
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| 234 | |
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| 235 | |
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| 236 | \end{center} |
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| 237 | \vspace{1.5cm} |
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| 238 | \begin{center} |
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| 239 | {\bf Abstract}\\ |
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| 240 | A water \v{C}erenkov detector project, of megaton scale, to be installed |
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| 241 | in the Fr\'ejus underground site and dedicated to nucleon decay, |
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| 242 | neutrinos from supernovae, solar and atmospheric neutrinos, as well as |
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| 243 | neutrinos from a super-beam and/or a beta-beam coming from CERN, is |
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| 244 | presented and compared with competitor projects in Japan and in the |
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| 245 | USA. The performances of the European project are discussed, including |
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| 246 | the possibility to measure the mixing angle $\theta_{13}$ and the |
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| 247 | CP-violating phase $\delta$. |
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| 248 | |
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| 249 | \end{center} |
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| 250 | |
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| 251 | \vspace{2.3cm} |
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| 252 | \end{titlepage} |
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| 253 | |
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| 254 | |
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| 255 | \newpage |
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| 256 | \tableofcontents |
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| 257 | \newpage |
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| 258 | |
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| 259 | \input{motivation} |
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| 260 | |
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| 261 | \newpage |
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| 262 | |
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| 263 | \section{Megaton Physics} |
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| 264 | \input{pdk_phy.tex} |
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| 265 | \input{snv_phy.tex} |
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| 266 | \input{osc_phy.tex} |
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| 267 | |
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| 268 | \newpage |
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| 269 | \input{undlab_detector.tex} |
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| 270 | \input{annex.tex} |
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| 271 | |
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| 272 | |
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| 273 | \newpage |
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| 274 | |
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| 275 | \section{Detector Performance} |
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| 276 | \label{sec:det} |
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| 277 | As mentioned above, we consider a massive water \v{C}erenkov detector |
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| 278 | {\`a} la UNO \cite{uno} and review the performances of such a detector for |
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| 279 | the main physics fields. |
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| 280 | |
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| 281 | \input{pdk_det.tex} |
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| 282 | \input{snv_det.tex} |
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| 283 | \input{osc_det.tex} |
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| 284 | \input{nusolar.tex} |
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| 285 | |
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| 286 | \newpage |
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| 287 | \input{conclusion.tex} |
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| 288 | |
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| 289 | \newpage |
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| 290 | \bibliography{Frejus} |
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| 291 | |
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| 292 | \end{document} |
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| 293 | |
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| 294 | |
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| 295 | |
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