[1208] | 1 | % \subsection{Neutron production} |
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| 2 | |
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| 3 | % \begin{figure}[tbp] |
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| 4 | % \resizebox{0.95\textwidth}{!} |
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| 5 | % { |
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| 6 | % \includegraphics{hadronic/theory_driven/BinaryCascade/dsde_256.eps} |
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| 7 | % } |
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| 8 | % \caption{1} |
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| 9 | % \label{nSigma} |
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| 10 | % \end{figure} |
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| 11 | % |
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| 12 | % \begin{figure}[tbp] |
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| 13 | % \resizebox{0.95\textwidth}{!} |
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| 14 | % { |
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| 15 | % \includegraphics{hadronic/theory_driven/BinaryCascade/dsdedt_256_7.5.eps} |
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| 16 | % } |
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| 17 | % \caption{2} |
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| 18 | % \label{nSigma} |
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| 19 | % \end{figure} |
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| 20 | % |
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| 21 | |
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| 22 | \begin{figure}[tbp] |
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| 23 | \begin{center} |
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| 24 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_al_113.eps} |
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| 25 | \end{center} |
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| 26 | \caption{ |
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| 27 | Double differential cross-section for neutrons produced in proton |
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| 28 | scattering off Aluminum. Proton incident energy was 113~MeV. |
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| 29 | } |
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| 30 | \label{nSigma.BC} |
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| 31 | \end{figure} |
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| 32 | |
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| 33 | \begin{figure}[tbp] |
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| 34 | \begin{center} |
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| 35 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_al_256.eps} |
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| 36 | \end{center} |
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| 37 | \caption{ |
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| 38 | Double differential cross-section for neutrons produced in proton |
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| 39 | scattering off Aluminum. Proton incident energy was 256~MeV. The points |
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| 40 | are data, the histogram is Binary Cascade prediction. |
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| 41 | } |
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| 42 | \label{dsdedt_al_256} |
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| 43 | \end{figure} |
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| 44 | |
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| 45 | \begin{figure}[tbp] |
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| 46 | \begin{center} |
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| 47 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_al_600.eps} |
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| 48 | \end{center} |
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| 49 | \caption{ |
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| 50 | Double differential cross-section for neutrons produced in proton |
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| 51 | scattering off Aluminum. Proton incident energy was 597~MeV. The points |
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| 52 | are data, the histogram is Binary Cascade prediction. |
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| 53 | } |
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| 54 | \label{dsdedt_al_600} |
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| 55 | \end{figure} |
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| 56 | |
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| 57 | \begin{figure}[tbp] |
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| 58 | \begin{center} |
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| 59 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_al_800.eps} |
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| 60 | \end{center} |
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| 61 | \caption{ |
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| 62 | Double differential cross-section for neutrons produced in proton |
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| 63 | scattering off Aluminum. Proton incident energy was 800~MeV. The points |
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| 64 | are data, the histogram is Binary Cascade prediction. |
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| 65 | } |
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| 66 | \label{dsdedt_al_800} |
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| 67 | \end{figure} |
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| 68 | |
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| 69 | \begin{figure}[tbp] |
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| 70 | \begin{center} |
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| 71 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_fe_113.eps} |
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| 72 | \end{center} |
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| 73 | \caption{ |
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| 74 | Double differential cross-section for neutrons produced in proton |
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| 75 | scattering off Iron. Proton incident energy was 113~MeV. The points |
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| 76 | are data, the histogram is Binary Cascade prediction. |
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| 77 | } |
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| 78 | \label{dsdedt_fe_113} |
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| 79 | \end{figure} |
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| 80 | |
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| 81 | \begin{figure}[tbp] |
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| 82 | \begin{center} |
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| 83 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_fe_256.eps} |
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| 84 | \end{center} |
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| 85 | \caption{ |
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| 86 | Double differential cross-section for neutrons produced in proton |
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| 87 | scattering off Iron. Proton incident energy was 256~MeV. The points |
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| 88 | are data, the histogram is Binary Cascade prediction. |
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| 89 | } |
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| 90 | \label{dsdedt_fe_256} |
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| 91 | \end{figure} |
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| 92 | |
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| 93 | \begin{figure}[tbp] |
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| 94 | \begin{center} |
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| 95 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_fe_600.eps} |
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| 96 | \end{center} |
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| 97 | \caption{ |
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| 98 | Double differential cross-section for neutrons produced in proton |
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| 99 | scattering off Iron. Proton incident energy was 597~MeV. The points |
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| 100 | are data, the histogram is Binary Cascade prediction. |
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| 101 | } |
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| 102 | \label{dsdedt_fe_600} |
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| 103 | \end{figure} |
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| 104 | |
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| 105 | \begin{figure}[tbp] |
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| 106 | \begin{center} |
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| 107 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_fe_800.eps} |
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| 108 | \end{center} |
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| 109 | \caption{ |
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| 110 | Double differential cross-section for neutrons produced in proton |
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| 111 | scattering off Iron. Proton incident energy was 800~MeV. The points |
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| 112 | are data, the histogram is Binary Cascade prediction. |
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| 113 | } |
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| 114 | \label{dsdedt_fe_800} |
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| 115 | \end{figure} |
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| 116 | |
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| 117 | \begin{figure}[tbp] |
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| 118 | \begin{center} |
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| 119 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_pb_113.eps} |
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| 120 | \end{center} |
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| 121 | \caption{ |
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| 122 | Double differential cross-section for neutrons produced in proton |
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| 123 | scattering off Lead. Proton incident energy was 113~MeV. The points |
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| 124 | are data, the histogram is Binary Cascade prediction. |
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| 125 | } |
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| 126 | \label{dsdedt_pb_113} |
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| 127 | \end{figure} |
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| 128 | |
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| 129 | \begin{figure}[tbp] |
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| 130 | \begin{center} |
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| 131 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_pb_256.eps} |
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| 132 | \end{center} |
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| 133 | \caption{ |
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| 134 | Double differential cross-section for neutrons produced in proton |
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| 135 | scattering off Lead. Proton incident energy was 256~MeV. The points |
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| 136 | are data, the histogram is Binary Cascade prediction. |
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| 137 | } |
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| 138 | \label{dsdedt_pb_256} |
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| 139 | \end{figure} |
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| 140 | |
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| 141 | \begin{figure}[tbp] |
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| 142 | \begin{center} |
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| 143 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_pb_600.eps} |
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| 144 | \end{center} |
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| 145 | \caption{ |
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| 146 | Double differential cross-section for neutrons produced in proton |
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| 147 | scattering off Lead. Proton incident energy was 597~MeV. The points |
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| 148 | are data, the histogram is Binary Cascade prediction. |
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| 149 | } |
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| 150 | \label{dsdedt_pb_600} |
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| 151 | \end{figure} |
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| 152 | |
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| 153 | \begin{figure}[tbp] |
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| 154 | \begin{center} |
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| 155 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/dsdedt_pb_800.eps} |
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| 156 | \end{center} |
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| 157 | \caption{ |
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| 158 | Double differential cross-section for neutrons produced in proton |
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| 159 | scattering off Lead. Proton incident energy was 800~MeV. The points |
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| 160 | are data, the histogram is Binary Cascade prediction. |
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| 161 | } |
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| 162 | \label{dsdedt_pb_800} |
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| 163 | \end{figure} |
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| 164 | |
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| 165 | \begin{figure}[tbp] |
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| 166 | \begin{center} |
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| 167 | \includegraphics[width=6.5cm]{hadronic/theory_driven/BinaryCascade/pi_45.eps} |
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| 168 | \end{center} |
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| 169 | \caption{ |
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| 170 | Double differential cross-section for pions produced at $45^\circ$ in proton |
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| 171 | scattering off various materials. Proton incident energy was 597~MeV in each |
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| 172 | case. The points are data, the histogram is Binary Cascade prediction. |
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| 173 | } |
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| 174 | \label{pi_45} |
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| 175 | \end{figure} |
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| 176 | |
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| 177 | |
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| 178 | % - Angle integrated energy distributions @ 160 MeV for Al, Zr, Pb |
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| 179 | % - Quasi-elastic peaks @ 256 MeV all materials |
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| 180 | % - double differentials: Al, Fe, Pb; all angles, 113, 160, 256, 595,800 MeV |
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