%% File for SLAC-PUB-5934, published in Phys. Rev. C (April, 1993) \input phyzzx \PHYSREV \twelvepoint \baselineskip 17pt \noindent Table I. Cross sections per deuteron nucleus for inelastic electron-deuteron scattering near break-up threshold. The beam energy $E$ and relative energy $E_{np}$ are evaluated at the center of the target. The errors include statistical and systematic contributions added in quadrature. \vskip .05in \input tables \def\tstrut{\vrule height 12pt depth 4pt width 0pt} \begintable \multispan{2} \tstrut\hfil $E=$0.734 GeV\hfil | \multispan{2} \tstrut\hfil $E=$0.843 GeV\hfil | \multispan{2} \tstrut\hfil $E=$0.885 GeV\hfil | \multispan{2} \tstrut\hfil $E=$0.934 GeV\hfil \nr $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ \nr (MeV) & (fb/sr-MeV) | (MeV) & (fb/sr-MeV) | (MeV) & (fb/sr-MeV) | (MeV) & (fb/sr-MeV) \nr \hfill -22.4 & \hfill $ 0.12\pm 0.29 $ | \hfill -25.4 & \hfill $ 0.01\pm 0.06 $ | \hfill -26.6 & \hfill $-0.02\pm 0.03 $ | \hfill -27.9 & \hfill $-0.02\pm 0.03 $ \nr \hfill -20.6 & \hfill $ 0.03\pm 0.29 $ | \hfill -23.3 & \hfill $ 0.01\pm 0.06 $ | \hfill -24.4 & \hfill $-0.01\pm 0.04 $ | \hfill -25.6 & \hfill $ 0.00\pm 0.03 $ \nr \hfill -18.7 & \hfill $-0.49\pm 0.25 $ | \hfill -21.2 & \hfill $-0.01\pm 0.06 $ | \hfill -22.2 & \hfill $-0.07\pm 0.04 $ | \hfill -23.3 & \hfill $-0.01\pm 0.03 $ \nr \hfill -16.9 & \hfill $-0.81\pm 0.31 $ | \hfill -19.1 & \hfill $-0.05\pm 0.06 $ | \hfill -20.0 & \hfill $-0.03\pm 0.04 $ | \hfill -20.9 & \hfill $ 0.01\pm 0.03 $ \nr \hfill -15.1 & \hfill $ 0.16\pm 0.35 $ | \hfill -17.0 & \hfill $ 0.03\pm 0.07 $ | \hfill -17.7 & \hfill $ 0.03\pm 0.04 $ | \hfill -18.6 & \hfill $ 0.00\pm 0.03 $ \nr \hfill -13.2 & \hfill $-0.32\pm 0.34 $ | \hfill -14.9 & \hfill $ 0.05\pm 0.08 $ | \hfill -15.5 & \hfill $-0.04\pm 0.04 $ | \hfill -16.2 & \hfill $ 0.01\pm 0.03 $ \nr \hfill -11.4 & \hfill $-0.18\pm 0.41 $ | \hfill -12.8 & \hfill $-0.05\pm 0.07 $ | \hfill -13.3 & \hfill $-0.05\pm 0.04 $ | \hfill -13.9 & \hfill $ 0.01\pm 0.03 $ \nr \hfill -9.6 & \hfill $ 0.27\pm 0.49 $ | \hfill -10.7 & \hfill $ 0.01\pm 0.08 $ | \hfill -11.1 & \hfill $-0.08\pm 0.06 $ | \hfill -11.6 & \hfill $ 0.02\pm 0.04 $ \nr \hfill -7.7 & \hfill $ 0.54\pm 0.59 $ | \hfill -8.6 & \hfill $ 0.00\pm 0.10 $ | \hfill -8.9 & \hfill $ 0.07\pm 0.09 $ | \hfill -9.2 & \hfill $ 0.04\pm 0.04 $ \nr \hfill -5.9 & \hfill $ 0.52\pm 0.56 $ | \hfill -6.4 & \hfill $ 0.04\pm 0.13 $ | \hfill -6.7 & \hfill $ 0.09\pm 0.10 $ | \hfill -6.9 & \hfill $ 0.09\pm 0.05 $ \nr \hfill -4.1 & \hfill $ 0.84\pm 0.59 $ | \hfill -4.3 & \hfill $ 0.14\pm 0.14 $ | \hfill -4.4 & \hfill $ 0.32\pm 0.12 $ | \hfill -4.6 & \hfill $ 0.12\pm 0.07 $ \nr \hfill -2.2 & \hfill $ 2.30\pm 0.64 $ | \hfill -2.2 & \hfill $ 0.52\pm 0.17 $ | \hfill -2.2 & \hfill $ 0.29\pm 0.12 $ | \hfill -2.2 & \hfill $ 0.21\pm 0.08 $ \nr \hfill -0.4 & \hfill $ 0.53\pm 0.56 $ | \hfill -0.1 & \hfill $ 0.57\pm 0.18 $ | \hfill 0.0 & \hfill $ 0.55\pm 0.14 $ | \hfill 0.1 & \hfill $ 0.33\pm 0.08 $ \nr \hfill 1.4 & \hfill $ 2.14\pm 0.73 $ | \hfill 2.0 & \hfill $ 0.62\pm 0.19 $ | \hfill 2.2 & \hfill $ 0.77\pm 0.14 $ | \hfill 2.4 & \hfill $ 0.42\pm 0.07 $ \nr \hfill 3.3 & \hfill $ 3.43\pm 0.87 $ | \hfill 4.1 & \hfill $ 1.00\pm 0.19 $ | \hfill 4.4 & \hfill $ 0.93\pm 0.15 $ | \hfill 4.8 & \hfill $ 0.43\pm 0.07 $ \nr \hfill 5.1 & \hfill $ 3.14\pm 1.04 $ | \hfill 6.2 & \hfill $ 1.50\pm 0.21 $ | \hfill 6.6 & \hfill $ 0.97\pm 0.17 $ | \hfill 7.1 & \hfill $ 0.56\pm 0.08 $ \nr \hfill 6.9 & \hfill $ 4.86\pm 1.11 $ | \hfill 8.3 & \hfill $ 1.24\pm 0.20 $ | \hfill 8.8 & \hfill $ 1.02\pm 0.19 $ | \hfill 9.4 & \hfill $ 0.64\pm 0.10 $ \nr \hfill 8.8 & \hfill $ 5.71\pm 1.18 $ | \hfill 10.4 & \hfill $ 1.45\pm 0.26 $ | \hfill 11.1 & \hfill $ 1.44\pm 0.24 $ | \hfill 11.8 & \hfill $ 0.72\pm 0.12 $ \nr \hfill 10.6 & \hfill $ 7.99\pm 1.29 $ | \hfill 12.5 & \hfill $ 1.69\pm 0.31 $ | \hfill 13.3 & \hfill $ 1.74\pm 0.26 $ | \hfill 14.1 & \hfill $ 0.79\pm 0.12 $ \nr \hfill 12.4 & \hfill $ 7.44\pm 1.27 $ | \hfill 14.6 & \hfill $ 1.88\pm 0.37 $ | \hfill 15.5 & \hfill $ 1.85\pm 0.27 $ | \hfill 16.5 & \hfill $ 1.04\pm 0.13 $ \nr \hfill 14.3 & \hfill $ 9.61\pm 1.45 $ | \hfill 16.7 & \hfill $ 3.12\pm 0.40 $ | \hfill 17.7 & \hfill $ 2.25\pm 0.29 $ | \hfill 18.8 & \hfill $ 1.15\pm 0.14 $ \nr \hfill 16.1 & \hfill $ 9.98\pm 1.55 $ | \hfill 18.9 & \hfill $ 2.77\pm 0.35 $ | \hfill 19.9 & \hfill $ 2.53\pm 0.31 $ | \hfill 21.1 & \hfill $ 1.01\pm 0.14 $ \nr \hfill 17.9 & \hfill $12.10\pm 1.76 $ | \hfill 21.0 & \hfill $ 3.21\pm 0.37 $ | \hfill 22.1 & \hfill $ 2.68\pm 0.32 $ | \hfill 23.5 & \hfill $ 1.41\pm 0.17 $ \nr \hfill 19.8 & \hfill $13.80\pm 1.83 $ | \hfill 23.1 & \hfill $ 2.95\pm 0.33 $ | \hfill 24.3 & \hfill $ 2.97\pm 0.33 $ | \hfill 25.8 & \hfill $ 1.47\pm 0.18 $ \nr \hfill 21.6 & \hfill $16.02\pm 1.89 $ | \hfill 25.2 & \hfill $ 3.58\pm 0.36 $ | \hfill 26.6 & \hfill $ 3.53\pm 0.35 $ | \hfill 28.1 & \hfill $ 1.82\pm 0.20 $ \nr \hfill 23.5 & \hfill $16.99\pm 1.91 $ | \hfill 27.3 & \hfill $ 4.44\pm 0.40 $ | \hfill 28.8 & \hfill $ 3.67\pm 0.35 $ | \hfill 30.5 & \hfill $ 1.84\pm 0.20 $ \endtable \vskip -.15in \hskip 4.9in {\it continued} \endpage \noindent Table I. continued. \vskip .15in \begintable \multispan{2} \tstrut\hfil $E=$1.020 GeV\hfil | \multispan{2} \tstrut\hfil $E=$1.102 GeV\hfil | \multispan{2} \tstrut\hfil $E=$1.201 GeV\hfil | \multispan{2} \tstrut\hfil $E=$1.279 GeV\hfil \nr $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ | $E_{np}$ & $d\sigma/d\Omega dE_{np}$ \nr (MeV) & (fb/sr-MeV) | (MeV & (fb/sr-MeV) | (MeV) & (fb/sr-MeV) | (MeV & (fb/sr-MeV) \nr \hfill -30.3 & \hfill $ 0.038\pm 0.012 $ | \hfill -32.6 & \hfill $ 0.001\pm 0.007 $ | \hfill -35.3 & \hfill $ 0.000\pm 0.004 $ | \hfill -37.4 & \hfill $-0.002\pm 0.002 $ \nr \hfill -27.7 & \hfill $ 0.001\pm 0.013 $ | \hfill -29.8 & \hfill $ 0.003\pm 0.008 $ | \hfill -32.3 & \hfill $-0.004\pm 0.004 $ | \hfill -34.2 & \hfill $-0.005\pm 0.002 $ \nr \hfill -25.2 & \hfill $ 0.006\pm 0.013 $ | \hfill -27.0 & \hfill $ 0.007\pm 0.010 $ | \hfill -29.3 & \hfill $ 0.007\pm 0.006 $ | \hfill -31.0 & \hfill $ 0.000\pm 0.003 $ \nr \hfill -22.6 & \hfill $-0.006\pm 0.013 $ | \hfill -24.3 & \hfill $-0.001\pm 0.009 $ | \hfill -26.3 & \hfill $-0.002\pm 0.006 $ | \hfill -27.8 & \hfill $-0.003\pm 0.002 $ \nr \hfill -20.1 & \hfill $ 0.014\pm 0.018 $ | \hfill -21.5 & \hfill $ 0.009\pm 0.009 $ | \hfill -23.3 & \hfill $ 0.013\pm 0.007 $ | \hfill -24.6 & \hfill $ 0.000\pm 0.003 $ \nr \hfill -17.5 & \hfill $ 0.004\pm 0.016 $ | \hfill -18.8 & \hfill $ 0.026\pm 0.011 $ | \hfill -20.3 & \hfill $ 0.002\pm 0.005 $ | \hfill -21.4 & \hfill $ 0.002\pm 0.004 $ \nr \hfill -15.0 & \hfill $-0.009\pm 0.016 $ | \hfill -16.0 & \hfill $-0.002\pm 0.008 $ | \hfill -17.3 & \hfill $-0.002\pm 0.005 $ | \hfill -18.2 & \hfill $ 0.003\pm 0.004 $ \nr \hfill -12.4 & \hfill $ 0.027\pm 0.019 $ | \hfill -13.3 & \hfill $ 0.016\pm 0.012 $ | \hfill -14.3 & \hfill $ 0.016\pm 0.008 $ | \hfill -15.0 & \hfill $ 0.005\pm 0.005 $ \nr \hfill -9.9 & \hfill $ 0.023\pm 0.021 $ | \hfill -10.5 & \hfill $ 0.019\pm 0.014 $ | \hfill -11.2 & \hfill $ 0.006\pm 0.008 $ | \hfill -11.8 & \hfill $ 0.010\pm 0.005 $ \nr \hfill -7.3 & \hfill $ 0.055\pm 0.024 $ | \hfill -7.7 & \hfill $ 0.034\pm 0.017 $ | \hfill -8.2 & \hfill $ 0.010\pm 0.009 $ | \hfill -8.6 & \hfill $ 0.004\pm 0.006 $ \nr \hfill -4.8 & \hfill $ 0.069\pm 0.026 $ | \hfill -5.0 & \hfill $ 0.049\pm 0.019 $ | \hfill -5.2 & \hfill $ 0.036\pm 0.010 $ | \hfill -5.4 & \hfill $ 0.025\pm 0.007 $ \nr \hfill -2.2 & \hfill $ 0.083\pm 0.032 $ | \hfill -2.2 & \hfill $ 0.068\pm 0.021 $ | \hfill -2.2 & \hfill $ 0.053\pm 0.012 $ | \hfill -2.2 & \hfill $ 0.028\pm 0.008 $ \nr \hfill 0.3 & \hfill $ 0.160\pm 0.040 $ | \hfill 0.5 & \hfill $ 0.098\pm 0.024 $ | \hfill 0.8 & \hfill $ 0.042\pm 0.011 $ | \hfill 1.0 & \hfill $ 0.047\pm 0.009 $ \nr \hfill 2.9 & \hfill $ 0.207\pm 0.041 $ | \hfill 3.3 & \hfill $ 0.157\pm 0.026 $ | \hfill 3.8 & \hfill $ 0.063\pm 0.013 $ | \hfill 4.2 & \hfill $ 0.042\pm 0.008 $ \nr \hfill 5.4 & \hfill $ 0.275\pm 0.047 $ | \hfill 6.0 & \hfill $ 0.145\pm 0.026 $ | \hfill 6.8 & \hfill $ 0.081\pm 0.014 $ | \hfill 7.4 & \hfill $ 0.067\pm 0.010 $ \nr \hfill 8.0 & \hfill $ 0.358\pm 0.054 $ | \hfill 8.8 & \hfill $ 0.183\pm 0.029 $ | \hfill 9.8 & \hfill $ 0.083\pm 0.016 $ | \hfill 10.6 & \hfill $ 0.041\pm 0.009 $ \nr \hfill 10.5 & \hfill $ 0.263\pm 0.054 $ | \hfill 11.6 & \hfill $ 0.199\pm 0.031 $ | \hfill 12.8 & \hfill $ 0.109\pm 0.018 $ | \hfill 13.8 & \hfill $ 0.069\pm 0.011 $ \nr \hfill 13.1 & \hfill $ 0.410\pm 0.065 $ | \hfill 14.3 & \hfill $ 0.262\pm 0.038 $ | \hfill 15.8 & \hfill $ 0.100\pm 0.017 $ | \hfill 17.0 & \hfill $ 0.078\pm 0.011 $ \nr \hfill 15.6 & \hfill $ 0.438\pm 0.067 $ | \hfill 17.1 & \hfill $ 0.263\pm 0.038 $ | \hfill 18.8 & \hfill $ 0.139\pm 0.020 $ | \hfill 20.2 & \hfill $ 0.071\pm 0.011 $ \nr \hfill 18.2 & \hfill $ 0.492\pm 0.066 $ | \hfill 19.8 & \hfill $ 0.259\pm 0.038 $ | \hfill 21.8 & \hfill $ 0.150\pm 0.020 $ | \hfill 23.4 & \hfill $ 0.062\pm 0.011 $ \nr \hfill 20.7 & \hfill $ 0.608\pm 0.074 $ | \hfill 22.6 & \hfill $ 0.334\pm 0.041 $ | \hfill 24.8 & \hfill $ 0.129\pm 0.022 $ | \hfill 26.5 & \hfill $ 0.091\pm 0.014 $ \nr \hfill 23.3 & \hfill $ 0.679\pm 0.074 $ | \hfill 25.4 & \hfill $ 0.365\pm 0.047 $ | \hfill 27.8 & \hfill $ 0.162\pm 0.024 $ | \hfill 29.8 & \hfill $ 0.100\pm 0.015 $ \nr \hfill 25.8 & \hfill $ 0.639\pm 0.074 $ | \hfill 28.1 & \hfill $ 0.352\pm 0.051 $ | \hfill 30.8 & \hfill $ 0.208\pm 0.027 $ | \hfill 33.0 & \hfill $ 0.103\pm 0.015 $ \nr \hfill 28.4 & \hfill $ 0.735\pm 0.076 $ | \hfill 30.9 & \hfill $ 0.422\pm 0.050 $ | \hfill 33.8 & \hfill $ 0.234\pm 0.028 $ | \hfill 36.2 & \hfill $ 0.144\pm 0.017 $ \nr \hfill 30.9 & \hfill $ 0.756\pm 0.076 $ | \hfill 33.6 & \hfill $ 0.502\pm 0.056 $ | \hfill 36.8 & \hfill $ 0.209\pm 0.027 $ | \hfill 39.3 & \hfill $ 0.134\pm 0.016 $ \nr \hfill 33.5 & \hfill $ 0.870\pm 0.077 $ | \hfill 36.4 & \hfill $ 0.556\pm 0.059 $ | \hfill 39.8 & \hfill $ 0.246\pm 0.029 $ | \hfill 42.5 & \hfill $ 0.114\pm 0.015 $ \endtable \endpage \noindent Table II. Ratio of the inelastic structure functions $W_1/W_2 $ for inelastic electron-deuteron scattering. The relative energy $E_{np}$ in units of MeV is evaluated at the target center, and the errors include both statistical and systematic contributions. \vskip .1in \begintable \multispan{2} \tstrut\hfil $=$1.36 (GeV/c)$^2$ \hfil | \multispan{2} \tstrut\hfil $=$1.84 (GeV/c)$^2$ \hfil | \multispan{2} \tstrut\hfil $=$2.33 (GeV/c)$^2$ \hfil \nr $E_{np} $ & $W_1/W_2$ | $E_{np} $ & $W_1/W_2$ | $E_{np} $ & $W_1/W_2$ \nr \hfill 9.4 & $0.178\pm 0.024 $ | \hfill 11.8 & $0.237\pm 0.035 $ | \hfill 14.3 & $0.386\pm 0.071 $ \nr \hfill 13.6 & $0.211\pm 0.027 $ | \hfill 16.9 & $0.317\pm 0.047 $ | \hfill 20.3 & $0.534\pm 0.094 $ \nr \hfill 17.8 & $0.320\pm 0.060 $ | \hfill 22.0 & $0.435\pm 0.068 $ | \hfill 26.3 & $0.525\pm 0.103 $ \nr \hfill 22.0 & $0.310\pm 0.061 $ | \hfill 27.1 & $0.441\pm 0.071 $ | \hfill 32.3 & $0.774\pm 0.147 $ \nr \hfill 26.2 & $0.368\pm 0.075 $ | \hfill 32.2 & $0.489\pm 0.077 $ | \hfill 38.3 & $0.730\pm 0.132 $ \nr \hfill 32.4 & $0.409\pm 0.065 $ | \hfill 38.5 & $0.428\pm 0.082 $ | \hfill 49.9 & $0.525\pm 0.129 $ \nr \hfill 40.3 & $0.521\pm 0.071 $ | \hfill 48.1 & $0.795\pm 0.113 $ | \hfill 61.4 & $0.734\pm 0.145 $ \nr \hfill 48.2 & $0.746\pm 0.089 $ | \hfill 57.6 & $0.541\pm 0.080 $ | \hfill 72.8 & $0.847\pm 0.147 $ \nr \hfill 56.1 & $0.812\pm 0.092 $ | \hfill 67.2 & $0.923\pm 0.115 $ | \hfill 85.6 & $0.711\pm 0.118 $ \nr \hfill 64.0 & $0.645\pm 0.073 $ | \hfill 76.8 & $0.743\pm 0.093 $ | \hfill 96.4 & $0.702\pm 0.106 $ \nr \hfill 71.9 & $0.796\pm 0.085 $ | \hfill 86.4 & $0.820\pm 0.097 $ | \hfill 107.1 & $0.857\pm 0.117 $ \nr \hfill 80.8 & $0.876\pm 0.114 $ | \hfill 96.0 & $0.827\pm 0.108 $ | \hfill 117.9 & $1.010\pm 0.130 $ \nr \hfill 88.3 & $0.931\pm 0.109 $ | \hfill 105.0 & $0.927\pm 0.108 $ | \hfill 128.7 & $0.764\pm 0.098 $ \nr \hfill 95.7 & $0.811\pm 0.095 $ | \hfill 114.0 & $0.931\pm 0.105 $ | \hfill 139.5 & $1.000\pm 0.120 $ \nr \hfill 103.1 & $0.892\pm 0.101 $ | \hfill 123.0 & $0.843\pm 0.094 $ | \hfill 151.5 & $0.877\pm 0.150 $ \nr \hfill 110.5 & $0.825\pm 0.094 $ | \hfill 132.0 & $0.856\pm 0.093 $ | \hfill 161.6 & $0.974\pm 0.140 $ \nr \hfill 118.0 & $0.924\pm 0.102 $ | \hfill 141.0 & $0.849\pm 0.090 $ | \hfill 171.7 & $1.050\pm 0.150 $ \nr \hfill 126.3 & $0.979\pm 0.122 $ | \hfill 151.3 & $1.010\pm 0.130 $ | \hfill 181.9 & $0.947\pm 0.130 $ \nr & | \hfill 159.8 & $1.110\pm 0.130 $ | \hfill 192.0 & $1.040\pm 0.130 $ \endtable \end