%%%\documentstyle[12pt,prl,aps]{revtex} \documentstyle[preprint,prl,aps]{revtex} \begin{document} %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%%%% \begin{tabular}{|c c p{0.6in} c c c|} \hline \multicolumn{6}{|p{4.3in}|}{Table I. Cross sections for inelastic electron scattering from protons for SLAC experiment NE11. The errors shown include statistical and point-to-point systematic uncertainties added in quadrature, but do not include an overall normalization error of about 1.8\%. Also shown are RC, the applied multiplicative radiative corrections to the raw cross sections after elastic tail subtraction, and RT, the subtracted elastic radiative tail. } \\ \hline & & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & RT & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ & \ (nb/sr-GeV)\ \\ & & & & & \\ \hline & & & & & \\ \multicolumn{6}{|c|}{$E=5.507$ GeV \ \ $\theta=15.146^\circ$} \\ & & & & & \\ 4.437 & 1.698 & 0.944 & 1.82 & 7.58 & $ 4.21\pm 1.04$ \\ 4.429 & 1.694 & 0.944 & 1.73 & 7.20 & $ 4.85\pm 1.06$ \\ 4.420 & 1.691 & 0.943 & 1.68 & 6.86 & $ 5.86\pm 1.08$ \\ 4.411 & 1.687 & 0.943 & 1.64 & 6.57 & $ 8.76\pm 1.13$ \\ 4.402 & 1.684 & 0.943 & 1.62 & 6.3 & $12.1\pm 1.2{\phantom{0}} $ \\ 4.393 & 1.681 & 0.942 & 1.60 & 6.0 & $15.4\pm 1.2{\phantom{0}} $ \\ 4.384 & 1.677 & 0.942 & 1.59 & 5.8 & $17.5\pm 1.3{\phantom{0}} $ \\ 4.375 & 1.674 & 0.941 & 1.58 & 5.6 & $22.5\pm 1.4{\phantom{0}} $ \\ 4.367 & 1.670 & 0.941 & 1.57 & 5.4 & $26.4\pm 1.5{\phantom{0}} $ \\ 4.358 & 1.667 & 0.940 & 1.56 & 5.3 & $32.9\pm 1.6{\phantom{0}} $ \\ 4.349 & 1.664 & 0.940 & 1.56 & 5.1 & $37.6\pm 1.7{\phantom{0}} $ \\ 4.340 & 1.660 & 0.940 & 1.55 & 5.0 & $48.5\pm 1.9{\phantom{0}} $ \\ 4.331 & 1.657 & 0.939 & 1.53 & 4.8 & $56.1\pm 2.0{\phantom{0}} $ \\ 4.322 & 1.654 & 0.939 & 1.51 & 4.7 & $62.2\pm 2.1{\phantom{0}} $ \\ 4.313 & 1.650 & 0.938 & 1.49 & 4.6 & $64.3\pm 2.1{\phantom{0}} $ \\ 4.304 & 1.647 & 0.938 & 1.45 & 4.5 & $68.1\pm 2.2{\phantom{0}} $ \\ 4.296 & 1.643 & 0.937 & 1.42 & 4.4 & $65.7\pm 2.1{\phantom{0}} $ \\ 4.287 & 1.640 & 0.937 & 1.38 & 4.3 & $63.6\pm 2.1{\phantom{0}} $ \\ 4.278 & 1.637 & 0.936 & 1.35 & 4.2 & $58.4\pm 2.1{\phantom{0}} $ \\ 4.269 & 1.633 & 0.936 & 1.31 & 4.1 & $57.1\pm 2.1{\phantom{0}} $ \\ 4.260 & 1.630 & 0.935 & 1.29 & 4.0 & $54.6\pm 2.1{\phantom{0}} $ \\ 4.252 & 1.626 & 0.935 & 1.26 & 4.0 & $50.3\pm 2.2{\phantom{0}} $ \\ 4.243 & 1.623 & 0.934 & 1.24 & 3.9 & $48.0\pm 2.3{\phantom{0}} $ \\ 4.234 & 1.620 & 0.934 & 1.23 & 3.8 & $52.1\pm 2.7{\phantom{0}} $ \\ 4.225 & 1.616 & 0.933 & 1.22 & 3.8 & $48.1\pm 2.9{\phantom{0}} $ \\ 4.216 & 1.613 & 0.933 & 1.21 & 3.7 & $45.8\pm 3.6{\phantom{0}} $ \\ 4.207 & 1.610 & 0.932 & 1.20 & 3.7 & $46.4\pm 4.7{\phantom{0}} $ \\ 4.198 & 1.606 & 0.932 & 1.19 & 3.6 & $50.8\pm 9.2{\phantom{0}} $ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c c|} \hline \multicolumn{6}{|p{4.3in}|}{Table I. Continued. } \\ \hline & & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & RT & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ & \ (nb/sr-GeV)\ \\ & & & & & \\ \hline & & & & & \\ \multicolumn{6}{|c|}{$E=5.507$ GeV \ \ $\theta=18.981^\circ$} \\ & & & & & \\ 4.060 & 2.431 & 0.906 & 2.10 & 1.450 & $ 0.549\pm 0.144$ \\ 4.048 & 2.424 & 0.905 & 1.80 & 1.337 & $ 0.814\pm 0.129$ \\ 4.035 & 2.417 & 0.904 & 1.70 & 1.24 & $ 1.21\pm 0.13$ \\ 4.024 & 2.409 & 0.903 & 1.64 & 1.17 & $ 1.76\pm 0.14$ \\ 4.011 & 2.402 & 0.903 & 1.61 & 1.10 & $ 2.13\pm 0.15$ \\ 3.999 & 2.395 & 0.902 & 1.59 & 1.04 & $ 2.94\pm 0.18$ \\ 3.987 & 2.388 & 0.901 & 1.58 & 0.99 & $ 4.20\pm 0.20$ \\ 3.975 & 2.380 & 0.900 & 1.57 & 0.95 & $ 6.19\pm 0.23$ \\ 3.963 & 2.373 & 0.899 & 1.55 & 0.91 & $ 7.57\pm 0.25$ \\ 3.951 & 2.366 & 0.898 & 1.53 & 0.87 & $ 9.30\pm 0.27$ \\ 3.938 & 2.359 & 0.898 & 1.50 & 0.8 & $10.8\pm 0.3{\phantom{0}} $ \\ 3.927 & 2.351 & 0.897 & 1.45 & 0.8 & $11.4\pm 0.3{\phantom{0}} $ \\ 3.914 & 2.344 & 0.896 & 1.40 & 0.8 & $11.3\pm 0.3{\phantom{0}} $ \\ 3.902 & 2.337 & 0.895 & 1.35 & 0.8 & $10.7\pm 0.3{\phantom{0}} $ \\ 3.890 & 2.330 & 0.894 & 1.31 & 0.75 & $ 9.99\pm 0.30$ \\ 3.878 & 2.322 & 0.893 & 1.28 & 0.73 & $ 9.38\pm 0.32$ \\ 3.866 & 2.315 & 0.892 & 1.26 & 0.71 & $ 9.53\pm 0.37$ \\ 3.854 & 2.308 & 0.891 & 1.24 & 0.70 & $ 9.08\pm 0.47$ \\ 3.842 & 2.300 & 0.890 & 1.23 & 0.68 & $ 8.84\pm 0.64$ \\ 3.830 & 2.293 & 0.889 & 1.22 & 0.67 & $ 7.57\pm 1.26$ \\ & & & & & \\ \multicolumn{6}{|c|}{$E=5.507$ GeV \ \ $\theta=22.805^\circ$} \\ & & & & & \\ 3.659 & 3.149 & 0.855 & 1.78 & 0.327 & $ 0.187\pm 0.026$ \\ 3.644 & 3.137 & 0.854 & 1.66 & 0.299 & $ 0.334\pm 0.027$ \\ 3.629 & 3.124 & 0.852 & 1.61 & 0.276 & $ 0.490\pm 0.033$ \\ 3.614 & 3.112 & 0.851 & 1.58 & 0.258 & $ 0.714\pm 0.038$ \\ 3.600 & 3.099 & 0.850 & 1.56 & 0.24 & $ 1.19\pm 0.05$ \\ 3.585 & 3.087 & 0.848 & 1.55 & 0.23 & $ 1.70\pm 0.06$ \\ 3.571 & 3.074 & 0.847 & 1.52 & 0.22 & $ 2.28\pm 0.07$ \\ 3.556 & 3.061 & 0.846 & 1.47 & 0.21 & $ 2.64\pm 0.07$ \\ 3.541 & 3.049 & 0.844 & 1.41 & 0.20 & $ 2.68\pm 0.07$ \\ 3.527 & 3.036 & 0.843 & 1.35 & 0.19 & $ 2.69\pm 0.07$ \\ 3.512 & 3.024 & 0.841 & 1.30 & 0.19 & $ 2.54\pm 0.08$ \\ 3.498 & 3.011 & 0.840 & 1.27 & 0.18 & $ 2.51\pm 0.09$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c c|} \hline \multicolumn{6}{|p{4.3in}|}{Table I. Continued. } \\ \hline & & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & RT & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ & \ (nb/sr-GeV)\ \\ & & & & & \\ \hline & & & & & \\ 3.483 & 2.999 & 0.839 & 1.26 & 0.18 & $ 2.66\pm 0.12$ \\ 3.468 & 2.986 & 0.837 & 1.25 & 0.18 & $ 2.26\pm 0.18$ \\ 3.454 & 2.973 & 0.836 & 1.24 & 0.17 & $ 2.08\pm 0.57$ \\ & & & & & \\ \multicolumn{6}{|c|}{$E=5.507$ GeV \ \ $\theta=26.823^\circ$} \\ & & & & & \\ 3.279 & 3.886 & 0.794 & 1.97 & 0.1056 & $0.0376\pm0.0086$ \\ 3.263 & 3.867 & 0.793 & 1.69 & 0.0938 & $0.0820\pm0.0080$ \\ 3.247 & 3.847 & 0.791 & 1.61 & 0.085 & $ 0.130\pm 0.009$ \\ 3.230 & 3.828 & 0.789 & 1.57 & 0.078 & $ 0.231\pm 0.011$ \\ 3.214 & 3.809 & 0.787 & 1.55 & 0.073 & $ 0.382\pm 0.013$ \\ 3.198 & 3.789 & 0.785 & 1.52 & 0.069 & $ 0.557\pm 0.015$ \\ 3.181 & 3.770 & 0.783 & 1.48 & 0.065 & $ 0.744\pm 0.017$ \\ 3.165 & 3.750 & 0.781 & 1.40 & 0.063 & $ 0.790\pm 0.018$ \\ 3.149 & 3.731 & 0.779 & 1.33 & 0.060 & $ 0.808\pm 0.019$ \\ 3.132 & 3.712 & 0.777 & 1.29 & 0.058 & $ 0.802\pm 0.021$ \\ 3.116 & 3.692 & 0.775 & 1.27 & 0.057 & $ 0.818\pm 0.028$ \\ 3.100 & 3.673 & 0.773 & 1.26 & 0.055 & $ 0.851\pm 0.046$ \\ 3.083 & 3.654 & 0.771 & 1.26 & 0.054 & $ 0.575\pm 0.171$ \\ & & & & & \\ \multicolumn{6}{|c|}{$E=9.800$ GeV \ \ $\theta=13.248^\circ$} \\ & & & & & \\ 7.545 & 3.936 & 0.942 & 2.11 & 0.427 & $ 0.234\pm 0.062$ \\ 7.525 & 3.925 & 0.941 & 1.80 & 0.374 & $ 0.391\pm 0.055$ \\ 7.504 & 3.914 & 0.940 & 1.72 & 0.335 & $ 0.672\pm 0.060$ \\ 7.483 & 3.903 & 0.940 & 1.67 & 0.30 & $ 1.07\pm 0.07$ \\ 7.462 & 3.892 & 0.939 & 1.65 & 0.28 & $ 1.76\pm 0.08$ \\ 7.441 & 3.882 & 0.938 & 1.63 & 0.26 & $ 2.64\pm 0.10$ \\ 7.420 & 3.871 & 0.938 & 1.58 & 0.24 & $ 3.43\pm 0.12$ \\ 7.399 & 3.860 & 0.937 & 1.50 & 0.23 & $ 3.53\pm 0.13$ \\ 7.379 & 3.849 & 0.936 & 1.43 & 0.22 & $ 3.53\pm 0.15$ \\ 7.358 & 3.838 & 0.936 & 1.39 & 0.20 & $ 3.29\pm 0.18$ \\ 7.337 & 3.827 & 0.935 & 1.36 & 0.20 & $ 3.57\pm 0.24$ \\ 7.316 & 3.816 & 0.934 & 1.35 & 0.19 & $ 3.34\pm 0.36$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c c|} \hline \multicolumn{6}{|p{4.3in}|}{Table I. Continued. } \\ \hline & & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & RT & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ & \ (nb/sr-GeV)\ \\ & & & & & \\ \hline & & & & & \\ \multicolumn{6}{|c|}{$E=9.800$ GeV \ \ $\theta=15.367^\circ$} \\ & & & & & \\ 7.016 & 4.916 & 0.914 & 1.99 & 0.1150 & $0.0844\pm0.0190$ \\ 6.988 & 4.896 & 0.913 & 1.74 & 0.096 & $ 0.183\pm 0.019$ \\ 6.958 & 4.876 & 0.912 & 1.67 & 0.083 & $ 0.360\pm 0.023$ \\ 6.929 & 4.855 & 0.911 & 1.63 & 0.074 & $ 0.595\pm 0.028$ \\ 6.900 & 4.835 & 0.909 & 1.56 & 0.067 & $ 0.880\pm 0.039$ \\ 6.870 & 4.815 & 0.908 & 1.46 & 0.06 & $ 1.04\pm 0.05$ \\ 6.842 & 4.794 & 0.907 & 1.40 & 0.057 & $ 0.994\pm 0.062$ \\ 6.812 & 4.774 & 0.905 & 1.38 & 0.054 & $ 0.908\pm 0.100$ \\ & & & & & \\ \multicolumn{6}{|c|}{$E=9.800$ GeV \ \ $\theta=17.516^\circ$} \\ & & & & & \\ 6.492 & 5.900 & 0.881 & 2.00 & 0.0381 & $0.0195\pm0.0070$ \\ 6.466 & 5.875 & 0.879 & 1.73 & 0.0319 & $0.0755\pm0.0078$ \\ 6.438 & 5.851 & 0.878 & 1.66 & 0.028 & $ 0.115\pm 0.009$ \\ 6.412 & 5.826 & 0.876 & 1.62 & 0.025 & $ 0.203\pm 0.011$ \\ 6.384 & 5.802 & 0.875 & 1.56 & 0.022 & $ 0.284\pm 0.014$ \\ 6.358 & 5.777 & 0.873 & 1.47 & 0.021 & $ 0.317\pm 0.018$ \\ 6.330 & 5.753 & 0.872 & 1.42 & 0.019 & $ 0.342\pm 0.023$ \\ 6.304 & 5.728 & 0.871 & 1.40 & 0.018 & $ 0.315\pm 0.033$ \\ 6.277 & 5.704 & 0.869 & 1.39 & 0.017 & $ 0.370\pm 0.114$ \\ & & & & & \\ \multicolumn{6}{|c|}{$E=9.800$ GeV \ \ $\theta=19.753^\circ$} \\ & & & & & \\ 5.944 & 6.855 & 0.839 & 1.73 & 0.0120 & $0.0330\pm0.0055$ \\ 5.919 & 6.826 & 0.837 & 1.65 & 0.0105 & $0.0382\pm0.0058$ \\ 5.895 & 6.797 & 0.836 & 1.60 & 0.0093 & $0.0582\pm0.0073$ \\ 5.869 & 6.769 & 0.834 & 1.55 & 0.009 & $ 0.102\pm 0.010$ \\ 5.845 & 6.740 & 0.832 & 1.47 & 0.008 & $ 0.110\pm 0.011$ \\ 5.820 & 6.712 & 0.831 & 1.43 & 0.007 & $ 0.125\pm 0.015$ \\ 5.795 & 6.683 & 0.829 & 1.41 & 0.007 & $ 0.154\pm 0.025$ \\ 5.770 & 6.655 & 0.827 & 1.40 & 0.007 & $ 0.168\pm 0.052$ \\ \hline \end{tabular} \eject %%%%%%%%%% END TABLE %%%%%%%%%%%%%% %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%%%% \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Per nucleon deuteron cross sections in the quasielastic and inelastic resonance regions from SLAC experiment NE11. The errors shown include statistical and point-to-point systematic uncertainties added in quadrature, but do not include an overall normalization error of about 2\%. Also shown are RC, the applied multiplicative radiative corrections to the raw cross sections. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ \multicolumn{5}{|c|}{$E=5.507$ GeV \ \ $\theta = 15.146^\circ$} \\ & & & & \\ 4.809 & 1.840 & .957 & 1.50 & $ 1.02\pm 0.23$ \\ 4.800 & 1.836 & .957 & 1.50 & $ 0.87\pm 0.20$ \\ 4.791 & 1.833 & .957 & 1.51 & $ 1.13\pm 0.17$ \\ 4.783 & 1.830 & .956 & 1.51 & $ 1.31\pm 0.17$ \\ 4.774 & 1.826 & .956 & 1.52 & $ 1.71\pm 0.17$ \\ 4.765 & 1.823 & .956 & 1.52 & $ 2.12\pm 0.19$ \\ 4.756 & 1.819 & .956 & 1.53 & $ 2.14\pm 0.18$ \\ 4.747 & 1.816 & .955 & 1.53 & $ 2.37\pm 0.17$ \\ 4.738 & 1.813 & .955 & 1.53 & $ 3.10\pm 0.18$ \\ 4.729 & 1.809 & .955 & 1.54 & $ 3.55\pm 0.19$ \\ 4.721 & 1.806 & .955 & 1.54 & $ 4.56\pm 0.21$ \\ 4.712 & 1.803 & .954 & 1.54 & $ 5.11\pm 0.22$ \\ 4.703 & 1.799 & .954 & 1.55 & $ 5.90\pm 0.25$ \\ 4.694 & 1.796 & .954 & 1.55 & $ 6.94\pm 0.27$ \\ 4.685 & 1.792 & .954 & 1.55 & $ 8.36\pm 0.29$ \\ 4.676 & 1.789 & .953 & 1.56 & $10.2\pm 0.3{\phantom{0}}$ \\ 4.667 & 1.786 & .953 & 1.56 & $11.7\pm 0.3{\phantom{0}}$ \\ 4.659 & 1.782 & .953 & 1.56 & $14.5\pm 0.4{\phantom{0}}$ \\ 4.650 & 1.779 & .952 & 1.56 & $17.5\pm 0.4{\phantom{0}}$ \\ 4.641 & 1.775 & .952 & 1.56 & $21.2\pm 0.5{\phantom{0}}$ \\ 4.632 & 1.772 & .952 & 1.56 & $25.3\pm 0.6{\phantom{0}}$ \\ 4.623 & 1.769 & .952 & 1.56 & $29.1\pm 0.6{\phantom{0}}$ \\ 4.614 & 1.765 & .951 & 1.55 & $35.7\pm 0.7{\phantom{0}}$ \\ 4.606 & 1.762 & .951 & 1.54 & $41.3\pm 0.8{\phantom{0}}$ \\ 4.597 & 1.759 & .951 & 1.53 & $47.0\pm 0.9{\phantom{0}}$ \\ 4.588 & 1.755 & .950 & 1.51 & $51.7\pm 1.1{\phantom{0}}$ \\ 4.579 & 1.752 & .950 & 1.48 & $53.1\pm 1.4{\phantom{0}}$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Continued. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ 4.570 & 1.748 & .950 & 1.44 & $54.0\pm 1.2$ \\ 4.561 & 1.745 & .949 & 1.40 & $53.1\pm 1.1$ \\ 4.552 & 1.742 & .949 & 1.36 & $49.9\pm 1.0$ \\ 4.544 & 1.738 & .949 & 1.31 & $45.6\pm 1.0$ \\ 4.535 & 1.735 & .948 & 1.27 & $40.2\pm 0.9$ \\ 4.526 & 1.731 & .948 & 1.22 & $35.5\pm 0.9$ \\ 4.517 & 1.728 & .948 & 1.17 & $31.4\pm 0.9$ \\ 4.508 & 1.725 & .947 & 1.13 & $27.8\pm 0.8$ \\ 4.499 & 1.721 & .947 & 1.10 & $24.9\pm 0.8$ \\ 4.490 & 1.718 & .946 & 1.07 & $22.8\pm 0.9$ \\ 4.482 & 1.714 & .946 & 1.04 & $20.9\pm 0.8$ \\ 4.473 & 1.711 & .946 & 1.03 & $19.2\pm 0.8$ \\ 4.464 & 1.708 & .945 & 1.02 & $18.0\pm 0.9$ \\ 4.455 & 1.704 & .945 & 1.01 & $17.8\pm 0.9$ \\ 4.446 & 1.701 & .945 & 1.02 & $17.7\pm 1.0$ \\ 4.437 & 1.698 & .944 & 1.03 & $17.3\pm 0.9$ \\ 4.429 & 1.694 & .944 & 1.05 & $17.2\pm 1.0$ \\ 4.420 & 1.691 & .943 & 1.07 & $18.1\pm 1.0$ \\ 4.411 & 1.687 & .943 & 1.10 & $19.8\pm 1.1$ \\ 4.402 & 1.684 & .943 & 1.13 & $20.9\pm 1.0$ \\ 4.393 & 1.681 & .942 & 1.15 & $22.5\pm 1.0$ \\ 4.384 & 1.677 & .942 & 1.18 & $24.2\pm 1.0$ \\ 4.375 & 1.674 & .941 & 1.20 & $25.5\pm 0.9$ \\ 4.367 & 1.670 & .941 & 1.22 & $27.3\pm 0.9$ \\ 4.358 & 1.667 & .940 & 1.24 & $28.5\pm 0.8$ \\ 4.349 & 1.664 & .940 & 1.25 & $31.6\pm 0.9$ \\ 4.340 & 1.660 & .940 & 1.26 & $33.9\pm 1.0$ \\ 4.331 & 1.657 & .939 & 1.27 & $34.8\pm 1.3$ \\ 4.322 & 1.654 & .939 & 1.27 & $38.0\pm 1.6$ \\ 4.313 & 1.650 & .938 & 1.27 & $39.1\pm 1.9$ \\ 4.304 & 1.647 & .938 & 1.26 & $40.2\pm 2.3$ \\ 4.296 & 1.643 & .937 & 1.26 & $40.7\pm 2.5$ \\ 4.287 & 1.640 & .937 & 1.25 & $40.0\pm 2.7$ \\ 4.278 & 1.637 & .936 & 1.24 & $41.3\pm 3.2$ \\ 4.269 & 1.633 & .936 & 1.23 & $42.7\pm 3.4$ \\ 4.260 & 1.630 & .935 & 1.22 & $42.5\pm 3.6$ \\ 4.252 & 1.626 & .935 & 1.20 & $40.7\pm 3.6$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Continued. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ 4.243 & 1.623 & .934 & 1.19 & $41.3\pm 3.8$ \\ 4.234 & 1.620 & .934 & 1.18 & $43.6\pm 4.1$ \\ 4.225 & 1.616 & .933 & 1.17 & $40.9\pm 4.1$ \\ 4.216 & 1.613 & .933 & 1.16 & $38.9\pm 4.3$ \\ 4.207 & 1.610 & .932 & 1.15 & $39.1\pm 4.5$ \\ 4.198 & 1.606 & .932 & 1.14 & $35.9\pm 5.9$ \\ & & & & \\ \multicolumn{5}{|c|}{$E=5.507$ GeV $\theta = 18.981^\circ$} \\ & & & & \\ 4.496 & 2.692 & .928 & 1.41 & $ .048\pm 0.017$ \\ 4.484 & 2.685 & .928 & 1.42 & $ .055\pm 0.016$ \\ 4.472 & 2.678 & .927 & 1.42 & $ .128\pm 0.021$ \\ 4.460 & 2.671 & .927 & 1.43 & $ .156\pm 0.022$ \\ 4.448 & 2.663 & .926 & 1.43 & $ .141\pm 0.019$ \\ 4.435 & 2.656 & .926 & 1.44 & $ .133\pm 0.019$ \\ 4.423 & 2.649 & .925 & 1.44 & $ .174\pm 0.022$ \\ 4.411 & 2.642 & .925 & 1.45 & $ .228\pm 0.024$ \\ 4.399 & 2.634 & .924 & 1.46 & $ .282\pm 0.025$ \\ 4.387 & 2.627 & .924 & 1.46 & $ .314\pm 0.027$ \\ 4.375 & 2.620 & .923 & 1.47 & $ .361\pm 0.030$ \\ 4.363 & 2.613 & .923 & 1.47 & $ .428\pm 0.032$ \\ 4.351 & 2.605 & .922 & 1.48 & $ .510\pm 0.032$ \\ 4.338 & 2.598 & .921 & 1.48 & $ .624\pm 0.032$ \\ 4.326 & 2.591 & .921 & 1.49 & $ .787\pm 0.035$ \\ 4.314 & 2.584 & .920 & 1.49 & $ .985\pm 0.037$ \\ 4.302 & 2.576 & .920 & 1.50 & $ 1.18\pm 0.04{\phantom{0}}$ \\ 4.290 & 2.569 & .919 & 1.50 & $ 1.44\pm 0.04{\phantom{0}}$ \\ 4.278 & 2.562 & .918 & 1.50 & $ 1.84\pm 0.05{\phantom{0}}$ \\ 4.266 & 2.555 & .918 & 1.51 & $ 2.26\pm 0.06{\phantom{0}}$ \\ 4.254 & 2.547 & .917 & 1.51 & $ 2.72\pm 0.07{\phantom{0}}$ \\ 4.242 & 2.540 & .916 & 1.51 & $ 3.37\pm 0.08{\phantom{0}}$ \\ 4.229 & 2.533 & .916 & 1.51 & $ 4.16\pm 0.10{\phantom{0}}$ \\ 4.217 & 2.525 & .915 & 1.50 & $ 5.10\pm 0.11{\phantom{0}}$ \\ 4.205 & 2.518 & .914 & 1.49 & $ 5.87\pm 0.13{\phantom{0}}$ \\ 4.193 & 2.511 & .914 & 1.46 & $ 6.68\pm 0.15{\phantom{0}}$ \\ 4.181 & 2.504 & .913 & 1.43 & $ 7.20\pm 0.20{\phantom{0}}$ \\ 4.169 & 2.496 & .912 & 1.40 & $ 7.23\pm 0.19{\phantom{0}}$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Continued. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ 4.157 & 2.489 & .912 & 1.36 & $ 7.08\pm 0.18$ \\ 4.145 & 2.482 & .911 & 1.31 & $ 6.61\pm 0.18$ \\ 4.132 & 2.475 & .910 & 1.26 & $ 6.04\pm 0.17$ \\ 4.120 & 2.467 & .910 & 1.21 & $ 5.32\pm 0.17$ \\ 4.108 & 2.460 & .909 & 1.17 & $ 4.75\pm 0.17$ \\ 4.096 & 2.453 & .908 & 1.14 & $ 4.31\pm 0.17$ \\ 4.084 & 2.446 & .907 & 1.11 & $ 3.94\pm 0.16$ \\ 4.072 & 2.438 & .907 & 1.10 & $ 3.71\pm 0.18$ \\ 4.060 & 2.431 & .906 & 1.10 & $ 3.51\pm 0.19$ \\ 4.048 & 2.424 & .905 & 1.11 & $ 3.64\pm 0.18$ \\ 4.035 & 2.417 & .904 & 1.12 & $ 3.71\pm 0.16$ \\ 4.024 & 2.409 & .903 & 1.14 & $ 4.01\pm 0.17$ \\ 4.011 & 2.402 & .903 & 1.17 & $ 4.18\pm 0.17$ \\ 3.999 & 2.395 & .902 & 1.19 & $ 4.53\pm 0.14$ \\ 3.987 & 2.388 & .901 & 1.21 & $ 5.00\pm 0.13$ \\ 3.975 & 2.380 & .900 & 1.23 & $ 5.40\pm 0.11$ \\ 3.963 & 2.373 & .899 & 1.24 & $ 5.67\pm 0.13$ \\ 3.951 & 2.366 & .898 & 1.24 & $ 5.99\pm 0.19$ \\ 3.938 & 2.359 & .898 & 1.25 & $ 6.44\pm 0.30$ \\ 3.927 & 2.351 & .897 & 1.24 & $ 6.88\pm 0.35$ \\ 3.914 & 2.344 & .896 & 1.24 & $ 7.23\pm 0.40$ \\ 3.902 & 2.337 & .895 & 1.23 & $ 7.45\pm 0.45$ \\ 3.890 & 2.330 & .894 & 1.22 & $ 7.62\pm 0.52$ \\ 3.878 & 2.322 & .893 & 1.21 & $ 7.85\pm 0.57$ \\ 3.866 & 2.315 & .892 & 1.20 & $ 7.92\pm 0.62$ \\ 3.854 & 2.308 & .891 & 1.19 & $ 8.09\pm 0.64$ \\ 3.842 & 2.300 & .890 & 1.18 & $ 7.95\pm 0.72$ \\ 3.830 & 2.293 & .889 & 1.17 & $ 8.14\pm 0.99$ \\ & & & & \\ \multicolumn{5}{|c|}{$E=5.507$ GeV \ \ $\theta = 22.805^\circ$} \\ & & & & \\ 3.936 & 3.388 & .877 & 1.43 & $ 0.172\pm 0.021$ \\ 3.921 & 3.376 & .876 & 1.44 & $ 0.205\pm 0.017$ \\ 3.907 & 3.363 & .875 & 1.44 & $ 0.256\pm 0.017$ \\ 3.892 & 3.351 & .874 & 1.45 & $ 0.331\pm 0.018$ \\ 3.877 & 3.338 & .873 & 1.45 & $ 0.424\pm 0.020$ \\ 3.863 & 3.326 & .871 & 1.46 & $ 0.542\pm 0.022$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Continued. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ 3.848 & 3.313 & .870 & 1.46 & $ 0.676\pm 0.025$ \\ 3.834 & 3.300 & .869 & 1.46 & $ 0.865\pm 0.030$ \\ 3.819 & 3.288 & .868 & 1.45 & $ 1.03\pm 0.04$ \\ 3.804 & 3.275 & .867 & 1.44 & $ 1.24\pm 0.04$ \\ 3.790 & 3.263 & .866 & 1.41 & $ 1.40\pm 0.04$ \\ 3.775 & 3.250 & .865 & 1.38 & $ 1.54\pm 0.05$ \\ 3.761 & 3.238 & .864 & 1.34 & $ 1.52\pm 0.05$ \\ 3.746 & 3.225 & .862 & 1.30 & $ 1.43\pm 0.05$ \\ 3.731 & 3.212 & .861 & 1.25 & $ 1.33\pm 0.05$ \\ 3.717 & 3.200 & .860 & 1.21 & $ 1.23\pm 0.05$ \\ 3.702 & 3.187 & .859 & 1.17 & $ 1.10\pm 0.04$ \\ 3.687 & 3.175 & .858 & 1.15 & $ 1.05\pm 0.05$ \\ 3.673 & 3.162 & .856 & 1.14 & $ 1.01\pm 0.05$ \\ 3.659 & 3.149 & .855 & 1.15 & $ 1.01\pm 0.05$ \\ 3.644 & 3.137 & .854 & 1.16 & $ 1.02\pm 0.05$ \\ 3.629 & 3.124 & .852 & 1.17 & $ 1.09\pm 0.05$ \\ 3.614 & 3.112 & .851 & 1.19 & $ 1.16\pm 0.04$ \\ 3.600 & 3.099 & .850 & 1.21 & $ 1.31\pm 0.03$ \\ 3.585 & 3.087 & .848 & 1.22 & $ 1.39\pm 0.04$ \\ 3.571 & 3.074 & .847 & 1.23 & $ 1.51\pm 0.04$ \\ 3.556 & 3.061 & .846 & 1.23 & $ 1.67\pm 0.07$ \\ 3.541 & 3.049 & .844 & 1.22 & $ 1.79\pm 0.08$ \\ 3.527 & 3.036 & .843 & 1.22 & $ 1.83\pm 0.09$ \\ 3.512 & 3.024 & .841 & 1.21 & $ 1.95\pm 0.11$ \\ 3.498 & 3.011 & .840 & 1.20 & $ 2.01\pm 0.14$ \\ 3.483 & 2.999 & .839 & 1.19 & $ 2.00\pm 0.15$ \\ 3.468 & 2.986 & .837 & 1.19 & $ 2.18\pm 0.18$ \\ 3.454 & 2.973 & .836 & 1.18 & $ 1.98\pm 0.38$ \\ & & & & \\ \multicolumn{5}{|c|}{$E=5.507$ GeV \ \ $\theta = 26.823^\circ$} \\ & & & & \\ 3.524 & 4.176 & .819 & 1.39 & $ 0.060\pm 0.009$ \\ 3.508 & 4.157 & .818 & 1.40 & $ 0.062\pm 0.007$ \\ 3.491 & 4.138 & .816 & 1.40 & $ 0.091\pm 0.007$ \\ 3.475 & 4.118 & .815 & 1.41 & $ 0.119\pm 0.008$ \\ 3.459 & 4.099 & .813 & 1.41 & $ 0.153\pm 0.008$ \\ 3.442 & 4.079 & .811 & 1.42 & $ 0.200\pm 0.010$ \\ \hline \end{tabular} \eject \begin{tabular}{|c c p{0.6in} c c|} \hline \multicolumn{5}{|p{3.4in}|}{Table II. Continued. } \\ \hline & & & & \\ $E^{\,\prime}$ & $Q^2$ & \ \ $\epsilon$\ \ & RC & $d\sigma /d\Omega dE^{\,\prime}$ \\ (GeV) & \ (GeV/c)$^2$\ & & & \ (nb/sr-GeV)\ \\ & & & & \\ \hline & & & & \\ 3.426 & 4.060 & .810 & 1.41 & $ 0.256\pm 0.011$ \\ 3.410 & 4.041 & .808 & 1.41 & $ 0.306\pm 0.013$ \\ 3.393 & 4.021 & .806 & 1.37 & $ 0.352\pm 0.015$ \\ 3.377 & 4.002 & .805 & 1.34 & $ 0.389\pm 0.017$ \\ 3.361 & 3.983 & .803 & 1.31 & $ 0.407\pm 0.016$ \\ 3.344 & 3.963 & .801 & 1.28 & $ 0.395\pm 0.018$ \\ 3.328 & 3.944 & .800 & 1.24 & $ 0.370\pm 0.018$ \\ 3.312 & 3.925 & .798 & 1.20 & $ 0.346\pm 0.015$ \\ 3.295 & 3.905 & .796 & 1.18 & $ 0.331\pm 0.019$ \\ 3.279 & 3.886 & .794 & 1.17 & $ 0.324\pm 0.018$ \\ 3.263 & 3.867 & .793 & 1.17 & $ 0.321\pm 0.016$ \\ 3.247 & 3.847 & .791 & 1.18 & $ 0.349\pm 0.016$ \\ 3.230 & 3.828 & .789 & 1.19 & $ 0.367\pm 0.013$ \\ 3.214 & 3.809 & .787 & 1.20 & $ 0.404\pm 0.014$ \\ 3.198 & 3.789 & .785 & 1.21 & $ 0.450\pm 0.011$ \\ 3.181 & 3.770 & .783 & 1.21 & $ 0.499\pm 0.018$ \\ 3.165 & 3.750 & .781 & 1.21 & $ 0.527\pm 0.021$ \\ 3.149 & 3.731 & .779 & 1.21 & $ 0.585\pm 0.022$ \\ 3.132 & 3.712 & .777 & 1.20 & $ 0.594\pm 0.034$ \\ 3.116 & 3.692 & .775 & 1.20 & $ 0.670\pm 0.043$ \\ 3.100 & 3.673 & .773 & 1.19 & $ 0.673\pm 0.052$ \\ 3.083 & 3.654 & .771 & 1.19 & $ 0.707\pm 0.174$ \\ \hline \end{tabular} \eject %%%%%%%%%% END TABLE %%%%%%%%%%%%%% %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%% \begin{tabular}{|c p{0.8in} c|} \hline \multicolumn{3}{|p{3.7in}|}{Table III. Resonance widths and masses used in fits. The index i = $\Delta$, 2, or 3 denotes the $\Delta$(1232) resonance and resonances 2 and 3, respectively. $Q^2$ is in units of (GeV/c)$^2$ } \\ \hline & & \\ $i$ & \hfill $\Gamma_i$ (GeV) &$M_i$ (GeV) \\ & & \\ \hline & & \\ $\Delta$ & \hfill 0.120\ \ \ & 1.232 \\ 2 & \hfill 0.074\ \ \ & 1.503 \\ 3 & \hfill 0.094\ \ \ & $ 1.677(1+0.0102Q^2 - 0.00084Q^4)$ \\ \hline \end{tabular} \vskip 0.5in %%%%%%%%%% END TABLE %%%%%%%%%%%%%% %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%% \begin{tabular}{|c c c c c c c|} \hline \multicolumn{7}{|p{6.3in}|}{Table IV. Results \cite{linda} of a global fit to the proton inelastic cross sections in units of $\mu$b and normalized to $[G_D(Q^2)]^2$. These coefficients are defined in Eqs. 3, 5, and 8. As described in the text, each coefficient has a polynomial dependence on $Q^2$ which is in (GeV/c)$^2$. The global fit gives a $\chi^2$ per 523 degrees of freedom of 1.56.} \\ \hline & & & & & &\\ $Q^{(2*n)}$ & $\vert F_\Delta \vert_n^2$ & $A_{2n}$ & $A_{3n}$ & $C_{1n}$ & $C_{2n}$ & $C_{3n}$ \\ & & & & & &\\ \hline & & & & & &\\ $Q^0$ &\ \phantom{$-$}1.396E+01\ &\ $-$3.153E+00\ &\ $-$4.540E$-$01\ &\ \phantom{$-$}3.167E+02\ &\ $-$1.711E+01\ &\ $-$1.836E+02\ \\ $Q^2$ &\ $-$2.879E+00\ &\ \phantom{$-$}2.933E+01\ &\ \phantom{$-$}1.935E+01\ &\ \phantom{$-$}1.490E+03\ &\ $-$5.320E+03\ &\ \phantom{$-$}4.144E+03\ \\ $Q^4$ & \ \phantom{$-$}1.587E$-$01\ & & & \ \phantom{$-$}6.120E+02\ & \ \phantom{$-$}5.364E+03\ & \ $-$4.890E+03\ \\ $Q^6$ & & & & \ \phantom{$-$}1.823E+01\ & \ $-$1.224E+03\ & \ \phantom{$-$}1.229E+03\ \\ $Q^8$ & & & & \ $-$6.437E+00\ & \ \phantom{$-$}7.816E+01\ & \ $-$7.934E+01\ \\ \hline \end{tabular} \eject %%%%%%%%%% END TABLE %%%%%%%%%%%%%% %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%% \begin{tabular}{|c|c|c|c|} \hline \multicolumn{4}{|p{4.3in}|}{Table V. NE11 and E133 $\Delta$(1232) transition form factor results determined from cross section data and normalized to $\mu_p G_D(Q^2)$. The first uncertainty is statistical, and the second is systematic including modeling and normalization uncertainties. Also shown are the $\chi^2$/dof values.} \\ \hline & & & \\ \ $Q^2$ (GeV/c)$^2$\ \ & \ \ $F_\Delta(Q^2)/ \mu_p G_D(Q^2)$\ & \ $\chi^2$/dof\ \ &\ Experiment\ \\ & & & \\ \hline & & & \\ 1.64 & \ \ 1.139$\pm$ 0.007 $\pm$ 0.023\ \ & 0.82 & NE11 \\ 2.34 & \ \ 1.014$\pm$ 0.007 $\pm$ 0.021\ \ & 1.01 & NE11 \\ 3.05 & \ \ 0.911$\pm$ 0.008 $\pm$ 0.022\ \ & 1.87 & NE11 \\ 3.75 & \ \ 0.804$\pm$ 0.008 $\pm$ 0.024\ \ & 5.30 & NE11 \\ 3.86 & \ \ 0.856$\pm$ 0.014 $\pm$ 0.038\ \ & 1.17 & NE11 \\ 4.82 & \ \ 0.732$\pm$ 0.020 $\pm$ 0.040\ \ & 1.92 & NE11 \\ 5.79 & \ \ 0.656$\pm$ 0.024 $\pm$ 0.047\ \ & 0.73 & NE11 \\ 6.75 & \ \ 0.513$\pm$ 0.052 $\pm$ 0.070\ \ & 1.27 & NE11 \\ 2.41 & \ \ 1.017$\pm$ 0.009 $\pm$ 0.068\ \ & 1.48 & E133 \\ 3.90 & \ \ 0.773$\pm$ 0.017 $\pm$ 0.069\ \ & 0.91 & E133 \\ 5.87 & \ \ 0.557$\pm$ 0.017 $\pm$ 0.131\ \ & 2.22 & E133 \\ 7.86 & \ \ 0.431$\pm$ 0.034 $\pm$ 0.174\ \ & 1.50 & E133 \\ 9.83 & \ \ 0.317$\pm$ 0.046 $\pm$ 0.245\ \ & 1.60 & E133 \\ \hline \end{tabular} \vskip 0.5in %%%%%%%%%% END TABLE %%%%%%%%%%%%%% %%%%%%%%%% BEGIN TABLE %%%%%%%%%%%% \begin{tabular}{|c|c|c|c|c|c |} \hline \multicolumn{6}{|p{6.1in}|}{Table VI. Ratios $\sigma_n/\sigma_p$ extracted from inelastic e-d cross sections in the region of the $\Delta$(1232) resonance for both resonant and non-resonant cross section components. The first uncertainty is statistical and the second is the quadratically combined systematic and modeling (dominant) uncertainties. The last line gives the combined $\chi^2$/dof for each fit.} \\ \hline & & & & &\\ $Q^2$& ${(\sigma_n/\sigma_p)}_{\Delta}$ & ${(\sigma_n/\sigma_p)}_{nres}$ & ${(\sigma_n/\sigma_p)}_{nres}$ & ${(\sigma_n/\sigma_p)}_{total}$ & Exp.\\ (${\rm GeV\over c}$)$^2$ & Fit I & Fit I & Fit II& Fit III& \\ & & & & & \\ \hline & & & & & \\ 1.64 &\ 0.81$\pm$0.10$\pm$0.05\ \ &\ 0.69$\pm$0.15$\pm$0.12\ \ &\ 0.41$\pm$0.04$\pm$0.15\ \ &\ 0.76$\pm$0.02$\pm$0.07\ \ &\ NE11\ \ \\ 2.34 &\ 0.73$\pm$0.13$\pm$0.09\ \ &\ 0.77$\pm$0.12$\pm$0.11\ \ &\ 0.53$\pm$0.04$\pm$0.14\ \ &\ 0.75$\pm$0.02$\pm$0.08\ \ &\ NE11\ \ \\ 3.05 &\ 0.63$\pm$0.22$\pm$0.10\ \ &\ 0.63$\pm$0.13$\pm$0.11\ \ &\ 0.43$\pm$0.04$\pm$0.13\ \ &\ 0.63$\pm$0.03$\pm$0.09\ \ &\ NE11\ \ \\ 3.75 &\ 0.14$\pm$0.35$\pm$0.21\ \ &\ 0.69$\pm$0.14$\pm$0.10\ \ &\ 0.37$\pm$0.04$\pm$0.12\ \ &\ 0.54$\pm$0.03$\pm$0.10\ \ &\ NE11\ \ \\ 2.41 &\ 0.71$\pm$0.05$\pm$0.16\ \ &\ 0.53$\pm$0.02$\pm$0.17\ \ &\ 0.45$\pm$0.02$\pm$0.15\ \ &\ 0.57$\pm$0.01$\pm$0.11\ \ &\ E133\ \ \\ 3.90 &\ 0.61$\pm$0.10$\pm$0.21\ \ &\ 0.45$\pm$0.03$\pm$0.13\ \ &\ 0.36$\pm$0.02$\pm$0.12\ \ &\ 0.48$\pm$0.01$\pm$0.10\ \ &\ E133\ \ \\ 5.87 &\ 0.83$\pm$0.24$\pm$0.43\ \ &\ 0.43$\pm$0.02$\pm$0.13\ \ &\ 0.42$\pm$0.02$\pm$0.11\ \ &\ 0.46$\pm$0.01$\pm$0.11\ \ &\ E133\ \ \\ 7.86 &\ 1.03$\pm$1.02$\pm$0.92\ \ &\ 0.46$\pm$0.04$\pm$0.13\ \ &\ 0.47$\pm$0.02$\pm$0.11\ \ &\ 0.48$\pm$0.02$\pm$0.11\ \ &\ E133\ \ \\ \hline $\chi^2$/dof & \multicolumn{2}{|c|}{1.41} & 1.52 & 1.40 & \\ \hline \end{tabular} \end{document}