%DATA FILES USED:
%/u/ea/robine/e143/steve/p29para_newrc2_newbp2
%/u/ea/robine/e143/steve/p29perp_newrc2_newbp2
%/u/ea/robine/e143/steve/d29para_newrc2_newbp2
%/u/ea/robine/e143/steve/d29perp_newrc2_newbp2
%/u/ea/robine/e143/steve/p16para_newrc2_newbp2
%/u/ea/robine/e143/steve/d16para_newrc2_newbp2
%/u/ea/robine/e143/steve/p9para_newrc2_newbp2 
%/u/ea/robine/e143/steve/d9para_newrc2_newbp2 

 %ENEGIES USED: MIN-MAX=  9.720 29.130
 %SPECTROMETERS USED: MIN-MAX   1   2
 % change ==  to  
 ==documentstyle[prl,aps]{revtex}
 ==begin{document}
 ==begin{table}[t] 
 ==caption{Proton    $A_==parallel$ and $A_==perp$ results with statistical errors for E=29.1  GeV at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ and $A^==perp_{rc}$ which were applied to the data. }
==label{tb:APpar29}
 ==begin{tabular}{rrrrrr}
$x$ & $<Q^2>$ &$A_==parallel$ & $A_{rc}^==parallel$ & $A_==perp$ & $A_{rc}^==perp$ ====
 ==hline
==multicolumn{6}{c}{$==theta=4.5^==circ$} ====
==hline
 0.028&  1.17& $-0.026==pm$ 0.054& $ 0.014 $& $ 0.031==pm$ 0.063& $ 0.004 $====
 0.031&  1.27& $ 0.048==pm$ 0.026& $ 0.014 $& $ 0.010==pm$ 0.032& $ 0.004 $====
 0.035&  1.40& $ 0.091==pm$ 0.019& $ 0.013 $& $ 0.012==pm$ 0.024& $ 0.004 $====
 0.039&  1.52& $ 0.060==pm$ 0.016& $ 0.012 $& $ 0.007==pm$ 0.020& $ 0.004 $====
 0.044&  1.65& $ 0.076==pm$ 0.015& $ 0.011 $& $ 0.004==pm$ 0.018& $ 0.004 $====
 0.049&  1.78& $ 0.083==pm$ 0.014& $ 0.010 $& $ 0.008==pm$ 0.017& $ 0.004 $====
 0.056&  1.92& $ 0.082==pm$ 0.013& $ 0.009 $& $ 0.003==pm$ 0.016& $ 0.004 $====
 0.063&  2.07& $ 0.082==pm$ 0.012& $ 0.008 $& $ 0.014==pm$ 0.015& $ 0.004 $====
 0.071&  2.22& $ 0.086==pm$ 0.011& $ 0.007 $& $ 0.012==pm$ 0.014& $ 0.004 $====
 0.079&  2.38& $ 0.102==pm$ 0.012& $ 0.006 $& $-0.009==pm$ 0.014& $ 0.004 $====
 0.090&  2.53& $ 0.081==pm$ 0.012& $ 0.005 $& $-0.006==pm$ 0.014& $ 0.004 $====
 0.101&  2.69& $ 0.114==pm$ 0.012& $ 0.004 $& $ 0.004==pm$ 0.014& $ 0.004 $====
 0.113&  2.84& $ 0.108==pm$ 0.013& $ 0.004 $& $-0.012==pm$ 0.015& $ 0.004 $====
 0.128&  3.00& $ 0.097==pm$ 0.013& $ 0.003 $& $ 0.010==pm$ 0.015& $ 0.004 $====
 0.144&  3.15& $ 0.086==pm$ 0.013& $ 0.003 $& $-0.031==pm$ 0.015& $ 0.004 $====
 0.162&  3.30& $ 0.113==pm$ 0.013& $ 0.003 $& $ 0.023==pm$ 0.016& $ 0.004 $====
 0.182&  3.45& $ 0.110==pm$ 0.014& $ 0.002 $& $-0.021==pm$ 0.016& $ 0.004 $====
 0.205&  3.59& $ 0.097==pm$ 0.014& $ 0.002 $& $ 0.043==pm$ 0.017& $ 0.004 $====
 0.230&  3.73& $ 0.118==pm$ 0.015& $ 0.002 $& $-0.005==pm$ 0.018& $ 0.004 $====
 0.259&  3.85& $ 0.107==pm$ 0.015& $ 0.002 $& $ 0.017==pm$ 0.019& $ 0.004 $====
 0.292&  3.98& $ 0.096==pm$ 0.016& $ 0.002 $& $-0.055==pm$ 0.020& $ 0.004 $====
 0.329&  4.09& $ 0.110==pm$ 0.018& $ 0.002 $& $-0.005==pm$ 0.022& $ 0.004 $====
 0.370&  4.20& $ 0.080==pm$ 0.020& $ 0.002 $& $ 0.012==pm$ 0.024& $ 0.003 $====
 0.416&  4.30& $ 0.140==pm$ 0.023& $ 0.002 $& $ 0.002==pm$ 0.028& $ 0.003 $====
 0.468&  4.40& $ 0.140==pm$ 0.026& $ 0.002 $& $-0.048==pm$ 0.032& $ 0.003 $====
 0.526&  4.47& $ 0.134==pm$ 0.031& $ 0.002 $& $-0.037==pm$ 0.038& $ 0.002 $====
 0.592&  4.55& $ 0.066==pm$ 0.037& $ 0.003 $& $-0.029==pm$ 0.045& $ 0.002 $====
 0.666&  4.63& $ 0.075==pm$ 0.045& $ 0.000 $& $-0.013==pm$ 0.055& $ 0.002 $====
 0.749&  4.70& $ 0.128==pm$ 0.062& $-0.007 $& $-0.114==pm$ 0.074& $ 0.004 $====
 ==hline
==multicolumn{6}{c}{$==theta=7.0^==circ$} ====
==hline
 0.071&  2.91& $ 0.261==pm$ 0.095& $ 0.018 $& $-0.122==pm$ 0.102& $ 0.006 $====
 0.079&  3.17& $ 0.159==pm$ 0.043& $ 0.015 $& $-0.002==pm$ 0.049& $ 0.006 $====
 0.090&  3.48& $ 0.115==pm$ 0.029& $ 0.012 $& $ 0.040==pm$ 0.034& $ 0.006 $====
 0.101&  3.79& $ 0.143==pm$ 0.024& $ 0.010 $& $-0.016==pm$ 0.027& $ 0.006 $====
 0.113&  4.11& $ 0.158==pm$ 0.022& $ 0.008 $& $ 0.011==pm$ 0.025& $ 0.006 $====
 0.128&  4.43& $ 0.164==pm$ 0.021& $ 0.006 $& $-0.026==pm$ 0.023& $ 0.006 $====
 0.144&  4.78& $ 0.159==pm$ 0.020& $ 0.005 $& $ 0.007==pm$ 0.022& $ 0.006 $====
 0.162&  5.13& $ 0.171==pm$ 0.019& $ 0.004 $& $ 0.018==pm$ 0.021& $ 0.006 $====
 0.182&  5.49& $ 0.192==pm$ 0.019& $ 0.003 $& $ 0.052==pm$ 0.021& $ 0.006 $====
 0.205&  5.86& $ 0.215==pm$ 0.019& $ 0.003 $& $ 0.012==pm$ 0.021& $ 0.006 $====
 0.230&  6.24& $ 0.150==pm$ 0.019& $ 0.002 $& $ 0.007==pm$ 0.022& $ 0.006 $====
 0.259&  6.60& $ 0.250==pm$ 0.020& $ 0.002 $& $ 0.001==pm$ 0.022& $ 0.006 $====
 0.292&  6.97& $ 0.197==pm$ 0.021& $ 0.002 $& $-0.023==pm$ 0.023& $ 0.005 $====
 0.329&  7.34& $ 0.195==pm$ 0.022& $ 0.002 $& $-0.012==pm$ 0.025& $ 0.005 $====
 0.370&  7.69& $ 0.190==pm$ 0.024& $ 0.002 $& $-0.018==pm$ 0.027& $ 0.005 $====
 0.416&  8.04& $ 0.244==pm$ 0.026& $ 0.002 $& $-0.009==pm$ 0.030& $ 0.004 $====
 0.468&  8.37& $ 0.223==pm$ 0.030& $ 0.002 $& $ 0.005==pm$ 0.034& $ 0.004 $====
 0.526&  8.68& $ 0.233==pm$ 0.034& $ 0.002 $& $-0.015==pm$ 0.039& $ 0.003 $====
 0.592&  8.99& $ 0.224==pm$ 0.041& $ 0.002 $& $-0.011==pm$ 0.047& $ 0.003 $====
 0.666&  9.26& $ 0.155==pm$ 0.051& $ 0.002 $& $-0.093==pm$ 0.063& $ 0.002 $====
 0.749&  9.53& $ 0.223==pm$ 0.069& $ 0.005 $& $-0.097==pm$ 0.094& $ 0.001 $====
==end{tabular}
 ==end{table}
 ==begin{table}[t] 
 ==caption{Proton    $A_==parallel$ results with statistical errors for E=16.2 GeV  at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ which were applied to the data. }
==label{tb:APpar16}
 ==begin{tabular}{rrrr}
$x$ & $<Q^2>$ &$A_==parallel$  & $A_{rc}^==parallel$              ==== 
 ==hline
==multicolumn{4}{c}{$==theta=4.5^==circ$} ====
==hline
 0.022&  0.47& $ 0.023==pm$ 0.024& $ 0.005$ ====
 0.024&  0.51& $ 0.066==pm$ 0.019& $ 0.005$ ====
 0.027&  0.55& $ 0.058==pm$ 0.018& $ 0.005$ ====
 0.031&  0.59& $ 0.054==pm$ 0.016& $ 0.005$ ====
 0.035&  0.64& $ 0.036==pm$ 0.015& $ 0.005$ ====
 0.039&  0.68& $ 0.041==pm$ 0.014& $ 0.005$ ====
 0.044&  0.73& $ 0.051==pm$ 0.013& $ 0.005$ ====
 0.049&  0.78& $ 0.074==pm$ 0.012& $ 0.005$ ====
 0.056&  0.83& $ 0.052==pm$ 0.012& $ 0.004$ ====
 0.063&  0.88& $ 0.068==pm$ 0.012& $ 0.004$ ====
 0.071&  0.92& $ 0.043==pm$ 0.012& $ 0.004$ ====
 0.079&  0.97& $ 0.046==pm$ 0.012& $ 0.003$ ====
 0.090&  1.01& $ 0.062==pm$ 0.012& $ 0.003$ ====
 0.101&  1.06& $ 0.071==pm$ 0.012& $ 0.003$ ====
 0.113&  1.10& $ 0.049==pm$ 0.012& $ 0.003$ ====
 0.128&  1.14& $ 0.060==pm$ 0.012& $ 0.002$ ====
 0.144&  1.18& $ 0.056==pm$ 0.012& $ 0.002$ ====
 0.162&  1.22& $ 0.068==pm$ 0.013& $ 0.002$ ====
 0.182&  1.26& $ 0.051==pm$ 0.013& $ 0.002$ ====
 0.205&  1.29& $ 0.060==pm$ 0.013& $ 0.002$ ====
 0.230&  1.32& $ 0.047==pm$ 0.014& $ 0.002$ ====
 0.259&  1.35& $ 0.041==pm$ 0.014& $ 0.002$ ====
 0.292&  1.38& $ 0.055==pm$ 0.015& $ 0.002$ ====
 0.329&  1.40& $ 0.043==pm$ 0.016& $ 0.003$ ====
 0.370&  1.43& $ 0.055==pm$ 0.017& $ 0.003$ ====
 0.416&  1.45& $ 0.079==pm$ 0.019& $ 0.000$ ====
 0.468&  1.46& $ 0.094==pm$ 0.021& $ 0.003$ ====
 0.527&  1.48& $ 0.082==pm$ 0.024& $ 0.010$ ====
 0.593&  1.49& $ 0.089==pm$ 0.028& $ 0.004$ ====
 0.668&  1.51& $ 0.052==pm$ 0.031& $-0.009$ ====
 0.752&  1.52& $ 0.258==pm$ 0.449& $-0.029$ ====
 ==hline
==multicolumn{4}{c}{$==theta=7.0^==circ$} ====
==hline
 0.044&  0.98& $ 0.072==pm$ 0.390& $ 0.012$ ====
 0.049&  1.06& $ 0.055==pm$ 0.078& $ 0.012$ ====
 0.056&  1.16& $ 0.091==pm$ 0.043& $ 0.011$ ====
 0.063&  1.26& $ 0.034==pm$ 0.031& $ 0.010$ ====
 0.071&  1.37& $ 0.092==pm$ 0.026& $ 0.009$ ====
 0.079&  1.47& $ 0.082==pm$ 0.023& $ 0.008$ ====
 0.090&  1.58& $ 0.113==pm$ 0.022& $ 0.007$ ====
 0.101&  1.69& $ 0.101==pm$ 0.021& $ 0.006$ ====
 0.113&  1.80& $ 0.108==pm$ 0.019& $ 0.005$ ====
 0.128&  1.91& $ 0.115==pm$ 0.018& $ 0.005$ ====
 0.144&  2.03& $ 0.120==pm$ 0.018& $ 0.004$ ====
 0.162&  2.14& $ 0.103==pm$ 0.017& $ 0.003$ ====
 0.182&  2.26& $ 0.105==pm$ 0.018& $ 0.003$ ====
 0.205&  2.36& $ 0.116==pm$ 0.018& $ 0.003$ ====
 0.230&  2.47& $ 0.136==pm$ 0.018& $ 0.002$ ====
 0.259&  2.57& $ 0.165==pm$ 0.019& $ 0.002$ ====
 0.292&  2.67& $ 0.159==pm$ 0.019& $ 0.002$ ====
 0.329&  2.76& $ 0.127==pm$ 0.020& $ 0.002$ ====
 0.370&  2.85& $ 0.157==pm$ 0.022& $ 0.002$ ====
 0.416&  2.94& $ 0.142==pm$ 0.023& $ 0.003$ ====
 0.468&  3.02& $ 0.150==pm$ 0.025& $ 0.003$ ====
 0.527&  3.08& $ 0.127==pm$ 0.029& $ 0.004$ ====
 0.593&  3.15& $ 0.070==pm$ 0.032& $-0.001$ ====
 0.668&  3.21& $ 0.136==pm$ 0.038& $ 0.003$ ====
 0.752&  3.27& $-0.280==pm$ 0.242& $ 0.009$ ====
==end{tabular}
 ==end{table}
 ==begin{table}[t] 
 ==caption{Proton    $A_==parallel$ results with statistical errors for E= 9.7 GeV  at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ which were applied to the data. }
==label{tb:APpar9}
 ==begin{tabular}{rrrr}
$x$ & $<Q^2>$ &$A_==parallel$  & $A_{rc}^==parallel$              ==== 
 ==hline
==multicolumn{4}{c}{$==theta=4.5^==circ$} ====
==hline
 0.028&  0.28& $ 0.021==pm$ 0.046& $ 0.003$ ====
 0.031&  0.30& $ 0.021==pm$ 0.022& $ 0.002$ ====
 0.035&  0.31& $ 0.048==pm$ 0.019& $ 0.002$ ====
 0.039&  0.33& $ 0.011==pm$ 0.017& $ 0.002$ ====
 0.044&  0.35& $ 0.046==pm$ 0.016& $ 0.001$ ====
 0.049&  0.36& $ 0.043==pm$ 0.016& $ 0.001$ ====
 0.056&  0.38& $ 0.040==pm$ 0.015& $ 0.001$ ====
 0.063&  0.40& $ 0.026==pm$ 0.015& $ 0.001$ ====
 0.071&  0.41& $ 0.030==pm$ 0.015& $ 0.001$ ====
 0.080&  0.43& $ 0.032==pm$ 0.015& $ 0.001$ ====
 0.090&  0.44& $ 0.018==pm$ 0.014& $ 0.000$ ====
 0.101&  0.45& $ 0.024==pm$ 0.014& $ 0.000$ ====
 0.113&  0.47& $ 0.041==pm$ 0.013& $ 0.000$ ====
 0.128&  0.48& $ 0.002==pm$ 0.013& $ 0.000$ ====
 0.144&  0.49& $ 0.002==pm$ 0.013& $ 0.000$ ====
 0.162&  0.50& $ 0.018==pm$ 0.013& $ 0.000$ ====
 0.182&  0.51& $ 0.024==pm$ 0.013& $-0.002$ ====
 0.205&  0.52& $ 0.015==pm$ 0.013& $-0.008$ ====
 0.231&  0.53& $ 0.054==pm$ 0.014& $-0.004$ ====
 0.259&  0.53& $ 0.047==pm$ 0.014& $ 0.015$ ====
 0.292&  0.54& $ 0.051==pm$ 0.016& $ 0.014$ ====
 0.329&  0.55& $ 0.020==pm$ 0.018& $ 0.001$ ====
 0.370&  0.55& $-0.002==pm$ 0.019& $-0.007$ ====
 0.417&  0.56& $-0.004==pm$ 0.021& $-0.015$ ====
 0.469&  0.56& $-0.034==pm$ 0.021& $-0.020$ ====
 0.527&  0.57& $ 0.007==pm$ 0.029& $-0.034$ ====
 0.594&  0.57& $-0.013==pm$ 0.064& $-0.043$ ====
 0.669&  0.57& $ 0.010==pm$ 0.179& $-0.039$ ====
 0.753&  0.58& $ 0.021==pm$ 0.214& $-0.036$ ====
 0.847&  0.58& $ 0.031==pm$ 0.257& $-0.032$ ====
 ==hline
==multicolumn{4}{c}{$==theta=7.0^==circ$} ====
==hline
 0.063&  0.60& $-0.013==pm$ 0.093& $ 0.003$ ====
 0.071&  0.64& $ 0.031==pm$ 0.038& $ 0.003$ ====
 0.080&  0.69& $ 0.076==pm$ 0.025& $ 0.003$ ====
 0.090&  0.74& $ 0.064==pm$ 0.019& $ 0.003$ ====
 0.101&  0.78& $ 0.057==pm$ 0.016& $ 0.003$ ====
 0.113&  0.82& $ 0.073==pm$ 0.015& $ 0.003$ ====
 0.128&  0.86& $ 0.048==pm$ 0.015& $ 0.003$ ====
 0.144&  0.90& $ 0.047==pm$ 0.014& $ 0.002$ ====
 0.162&  0.93& $ 0.065==pm$ 0.013& $ 0.002$ ====
 0.182&  0.97& $ 0.087==pm$ 0.013& $ 0.002$ ====
 0.205&  1.00& $ 0.068==pm$ 0.013& $ 0.002$ ====
 0.231&  1.03& $ 0.084==pm$ 0.013& $ 0.002$ ====
 0.259&  1.06& $ 0.070==pm$ 0.013& $ 0.003$ ====
 0.292&  1.09& $ 0.055==pm$ 0.013& $ 0.004$ ====
 0.329&  1.12& $ 0.088==pm$ 0.014& $ 0.005$ ====
 0.370&  1.14& $ 0.088==pm$ 0.014& $-0.004$ ====
 0.417&  1.16& $ 0.082==pm$ 0.016& $ 0.001$ ====
 0.469&  1.18& $ 0.084==pm$ 0.016& $ 0.018$ ====
 0.527&  1.21& $ 0.086==pm$ 0.018& $ 0.010$ ====
 0.594&  1.22& $-0.001==pm$ 0.018& $-0.004$ ====
 0.669&  1.23& $ 0.022==pm$ 0.018& $-0.026$ ====
 0.753&  1.25& $-0.044==pm$ 0.047& $-0.061$ ====
 0.847&  1.26& $-0.018==pm$ 0.149& $-0.064$ ====
==end{tabular}
 ==end{table}
 ==begin{table}[t] 
 ==caption{Deuteron  $A_==parallel$ and $A_==perp$ results with statistical errors for E=29.1  GeV at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ and $A^==perp_{rc}$ which were applied to the data. }
==label{tb:ADpar29}
 ==begin{tabular}{rrrrrr}
$x$ & $<Q^2>$ &$A_==parallel$ & $A_{rc}^==parallel$ & $A_==perp$ & $A_{rc}^==perp$ ====
 ==hline
==multicolumn{6}{c}{$==theta=4.5^==circ$} ====
==hline
 0.028&  1.17& $-0.042==pm$ 0.075& $-0.004 $& $-0.138==pm$ 0.175& $ 0.002 $====
 0.031&  1.27& $ 0.035==pm$ 0.030& $-0.004 $& $-0.114==pm$ 0.146& $ 0.002 $====
 0.035&  1.40& $ 0.004==pm$ 0.021& $-0.004 $& $ 0.060==pm$ 0.083& $ 0.002 $====
 0.039&  1.52& $ 0.043==pm$ 0.019& $-0.004 $& $ 0.038==pm$ 0.046& $ 0.002 $====
 0.044&  1.65& $-0.011==pm$ 0.017& $-0.004 $& $ 0.050==pm$ 0.038& $ 0.002 $====
 0.049&  1.78& $-0.009==pm$ 0.016& $-0.004 $& $ 0.022==pm$ 0.034& $ 0.002 $====
 0.056&  1.92& $ 0.012==pm$ 0.015& $-0.003 $& $-0.043==pm$ 0.031& $ 0.002 $====
 0.063&  2.07& $ 0.010==pm$ 0.014& $-0.003 $& $-0.040==pm$ 0.029& $ 0.002 $====
 0.071&  2.22& $ 0.014==pm$ 0.013& $-0.003 $& $ 0.009==pm$ 0.028& $ 0.002 $====
 0.079&  2.38& $ 0.023==pm$ 0.013& $-0.003 $& $-0.009==pm$ 0.029& $ 0.002 $====
 0.090&  2.53& $ 0.038==pm$ 0.014& $-0.003 $& $ 0.032==pm$ 0.029& $ 0.002 $====
 0.101&  2.69& $ 0.028==pm$ 0.014& $-0.003 $& $-0.031==pm$ 0.030& $ 0.002 $====
 0.113&  2.84& $ 0.037==pm$ 0.015& $-0.002 $& $ 0.012==pm$ 0.031& $ 0.002 $====
 0.128&  3.00& $ 0.079==pm$ 0.015& $-0.002 $& $-0.001==pm$ 0.032& $ 0.002 $====
 0.144&  3.15& $ 0.053==pm$ 0.016& $-0.002 $& $-0.023==pm$ 0.033& $ 0.002 $====
 0.162&  3.30& $ 0.046==pm$ 0.016& $-0.001 $& $ 0.043==pm$ 0.035& $ 0.002 $====
 0.182&  3.45& $ 0.054==pm$ 0.017& $-0.001 $& $-0.042==pm$ 0.036& $ 0.002 $====
 0.205&  3.59& $ 0.049==pm$ 0.017& $ 0.000 $& $-0.013==pm$ 0.038& $ 0.002 $====
 0.230&  3.73& $ 0.020==pm$ 0.019& $ 0.000 $& $ 0.008==pm$ 0.040& $ 0.002 $====
 0.259&  3.85& $ 0.021==pm$ 0.020& $ 0.000 $& $ 0.095==pm$ 0.043& $ 0.002 $====
 0.292&  3.98& $ 0.054==pm$ 0.021& $ 0.001 $& $-0.016==pm$ 0.047& $ 0.002 $====
 0.329&  4.09& $ 0.078==pm$ 0.023& $ 0.001 $& $-0.025==pm$ 0.052& $ 0.002 $====
 0.370&  4.20& $ 0.072==pm$ 0.026& $ 0.001 $& $-0.026==pm$ 0.059& $ 0.002 $====
 0.416&  4.30& $ 0.063==pm$ 0.030& $ 0.001 $& $-0.050==pm$ 0.068& $ 0.001 $====
 0.468&  4.40& $ 0.010==pm$ 0.036& $ 0.001 $& $-0.071==pm$ 0.081& $ 0.001 $====
 0.526&  4.47& $ 0.065==pm$ 0.043& $ 0.001 $& $ 0.077==pm$ 0.098& $ 0.001 $====
 0.592&  4.55& $ 0.057==pm$ 0.052& $ 0.001 $& $-0.116==pm$ 0.120& $ 0.001 $====
 0.666&  4.62& $ 0.023==pm$ 0.066& $-0.002 $& $ 0.160==pm$ 0.150& $ 0.002 $====
 0.749&  4.70& $-0.190==pm$ 0.091& $-0.006 $& $ 0.150==pm$ 0.203& $ 0.004 $====
 ==hline
==multicolumn{6}{c}{$==theta=7.0^==circ$} ====
==hline
 0.071&  2.91& $ 0.044==pm$ 0.108& $-0.004 $& $ 0.088==pm$ 0.237& $ 0.003 $====
 0.079&  3.17& $-0.020==pm$ 0.049& $-0.004 $& $ 0.081==pm$ 0.094& $ 0.003 $====
 0.090&  3.48& $ 0.044==pm$ 0.033& $-0.004 $& $-0.024==pm$ 0.062& $ 0.003 $====
 0.101&  3.79& $ 0.044==pm$ 0.027& $-0.004 $& $ 0.075==pm$ 0.050& $ 0.003 $====
 0.113&  4.11& $ 0.023==pm$ 0.025& $-0.004 $& $-0.036==pm$ 0.046& $ 0.003 $====
 0.128&  4.44& $ 0.053==pm$ 0.023& $-0.003 $& $-0.014==pm$ 0.043& $ 0.003 $====
 0.144&  4.78& $ 0.110==pm$ 0.023& $-0.003 $& $-0.038==pm$ 0.041& $ 0.003 $====
 0.162&  5.13& $ 0.051==pm$ 0.022& $-0.003 $& $-0.027==pm$ 0.041& $ 0.003 $====
 0.182&  5.49& $ 0.133==pm$ 0.022& $-0.002 $& $ 0.035==pm$ 0.040& $ 0.003 $====
 0.205&  5.86& $ 0.067==pm$ 0.022& $-0.002 $& $-0.085==pm$ 0.041& $ 0.003 $====
 0.230&  6.23& $ 0.088==pm$ 0.023& $-0.001 $& $-0.056==pm$ 0.043& $ 0.003 $====
 0.259&  6.60& $ 0.051==pm$ 0.024& $ 0.000 $& $ 0.065==pm$ 0.045& $ 0.003 $====
 0.292&  6.97& $ 0.102==pm$ 0.026& $ 0.000 $& $-0.028==pm$ 0.048& $ 0.003 $====
 0.329&  7.33& $ 0.108==pm$ 0.028& $ 0.001 $& $-0.034==pm$ 0.052& $ 0.002 $====
 0.370&  7.69& $ 0.143==pm$ 0.030& $ 0.001 $& $-0.024==pm$ 0.057& $ 0.002 $====
 0.416&  8.03& $ 0.089==pm$ 0.034& $ 0.001 $& $-0.018==pm$ 0.064& $ 0.002 $====
 0.468&  8.37& $ 0.125==pm$ 0.039& $ 0.000 $& $-0.003==pm$ 0.073& $ 0.002 $====
 0.526&  8.67& $ 0.172==pm$ 0.046& $ 0.000 $& $-0.023==pm$ 0.086& $ 0.002 $====
 0.592&  8.98& $ 0.094==pm$ 0.056& $-0.001 $& $ 0.235==pm$ 0.108& $ 0.002 $====
 0.666&  9.26& $ 0.086==pm$ 0.070& $-0.001 $& $-0.125==pm$ 0.147& $ 0.002 $====
 0.749&  9.52& $ 0.193==pm$ 0.096& $ 0.000 $& $-0.068==pm$ 0.212& $ 0.002 $====
==end{tabular}
 ==end{table}
 ==begin{table}[t] 
 ==caption{Deuteron  $A_==parallel$ results with statistical errors for E=16.2 GeV  at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ which were applied to the data. }
==label{tb:ADpar16}
 ==begin{tabular}{rrrr}
$x$ & $<Q^2>$ &$A_==parallel$  & $A_{rc}^==parallel$              ==== 
 ==hline
==multicolumn{4}{c}{$==theta=4.5^==circ$} ====
==hline
 0.022&  0.47& $-0.018==pm$ 0.064& $-0.006$ ====
 0.024&  0.51& $-0.035==pm$ 0.049& $-0.006$ ====
 0.027&  0.55& $-0.012==pm$ 0.045& $-0.005$ ====
 0.031&  0.59& $ 0.012==pm$ 0.041& $-0.005$ ====
 0.035&  0.64& $-0.009==pm$ 0.038& $-0.004$ ====
 0.039&  0.68& $ 0.056==pm$ 0.034& $-0.004$ ====
 0.044&  0.73& $-0.021==pm$ 0.028& $-0.004$ ====
 0.049&  0.78& $ 0.046==pm$ 0.026& $-0.003$ ====
 0.056&  0.83& $ 0.003==pm$ 0.025& $-0.003$ ====
 0.063&  0.87& $ 0.021==pm$ 0.025& $-0.003$ ====
 0.071&  0.92& $ 0.026==pm$ 0.025& $-0.003$ ====
 0.079&  0.97& $-0.016==pm$ 0.025& $-0.002$ ====
 0.090&  1.01& $ 0.038==pm$ 0.025& $-0.002$ ====
 0.101&  1.06& $ 0.019==pm$ 0.025& $-0.002$ ====
 0.113&  1.10& $ 0.016==pm$ 0.025& $-0.001$ ====
 0.128&  1.14& $ 0.063==pm$ 0.025& $-0.001$ ====
 0.144&  1.18& $ 0.050==pm$ 0.025& $-0.001$ ====
 0.162&  1.22& $-0.025==pm$ 0.025& $-0.001$ ====
 0.182&  1.25& $ 0.043==pm$ 0.026& $ 0.000$ ====
 0.205&  1.29& $ 0.042==pm$ 0.027& $ 0.000$ ====
 0.230&  1.32& $ 0.016==pm$ 0.027& $ 0.000$ ====
 0.259&  1.35& $ 0.022==pm$ 0.029& $ 0.001$ ====
 0.292&  1.37& $ 0.062==pm$ 0.031& $ 0.001$ ====
 0.329&  1.40& $ 0.023==pm$ 0.033& $ 0.001$ ====
 0.370&  1.42& $-0.031==pm$ 0.036& $ 0.001$ ====
 0.416&  1.44& $ 0.013==pm$ 0.040& $-0.001$ ====
 0.468&  1.46& $ 0.089==pm$ 0.045& $ 0.001$ ====
 0.527&  1.48& $ 0.014==pm$ 0.053& $ 0.003$ ====
 0.593&  1.49& $ 0.071==pm$ 0.063& $-0.002$ ====
 0.668&  1.50& $ 0.037==pm$ 0.076& $-0.013$ ====
 ==hline
==multicolumn{4}{c}{$==theta=7.0^==circ$} ====
==hline
 0.049&  1.06& $-0.075==pm$ 0.201& $-0.005$ ====
 0.056&  1.16& $ 0.062==pm$ 0.106& $-0.005$ ====
 0.063&  1.26& $-0.003==pm$ 0.075& $-0.004$ ====
 0.071&  1.36& $ 0.054==pm$ 0.060& $-0.004$ ====
 0.079&  1.47& $-0.073==pm$ 0.054& $-0.004$ ====
 0.090&  1.58& $ 0.121==pm$ 0.049& $-0.004$ ====
 0.101&  1.69& $ 0.054==pm$ 0.046& $-0.003$ ====
 0.113&  1.80& $ 0.027==pm$ 0.041& $-0.003$ ====
 0.128&  1.91& $ 0.018==pm$ 0.038& $-0.002$ ====
 0.144&  2.03& $ 0.039==pm$ 0.036& $-0.002$ ====
 0.162&  2.14& $ 0.060==pm$ 0.036& $-0.002$ ====
 0.182&  2.25& $ 0.097==pm$ 0.036& $-0.001$ ====
 0.205&  2.36& $ 0.045==pm$ 0.036& $-0.001$ ====
 0.230&  2.47& $ 0.041==pm$ 0.038& $ 0.000$ ====
 0.259&  2.57& $ 0.041==pm$ 0.039& $ 0.000$ ====
 0.292&  2.67& $ 0.115==pm$ 0.040& $ 0.001$ ====
 0.329&  2.76& $ 0.160==pm$ 0.042& $ 0.001$ ====
 0.370&  2.85& $ 0.039==pm$ 0.045& $ 0.001$ ====
 0.416&  2.93& $ 0.055==pm$ 0.049& $ 0.001$ ====
 0.468&  3.01& $ 0.168==pm$ 0.054& $ 0.001$ ====
 0.527&  3.08& $ 0.139==pm$ 0.062& $ 0.001$ ====
 0.593&  3.15& $ 0.055==pm$ 0.073& $-0.002$ ====
 0.668&  3.21& $-0.013==pm$ 0.088& $-0.001$ ====
==end{tabular}
 ==end{table}
 ==begin{table}[t] 
 ==caption{Deuteron  $A_==parallel$ results with statistical errors for E= 9.7 GeV  at the measured $Q^2$ in (GeV/c)$^2$.  Also shown are the radiative corrections $A_{rc}^==parallel$ which were applied to the data. }
==label{tb:ADpar9}
 ==begin{tabular}{rrrr}
$x$ & $<Q^2>$ &$A_==parallel$  & $A_{rc}^==parallel$              ==== 
 ==hline
==multicolumn{4}{c}{$==theta=4.5^==circ$} ====
==hline
 0.028&  0.28& $ 0.053==pm$ 0.069& $-0.005$ ====
 0.031&  0.30& $-0.067==pm$ 0.034& $-0.005$ ====
 0.035&  0.31& $-0.014==pm$ 0.028& $-0.004$ ====
 0.039&  0.33& $ 0.017==pm$ 0.025& $-0.004$ ====
 0.044&  0.35& $ 0.001==pm$ 0.024& $-0.004$ ====
 0.050&  0.36& $ 0.022==pm$ 0.023& $-0.004$ ====
 0.056&  0.38& $-0.017==pm$ 0.022& $-0.003$ ====
 0.063&  0.40& $-0.002==pm$ 0.021& $-0.003$ ====
 0.071&  0.41& $ 0.032==pm$ 0.022& $-0.003$ ====
 0.080&  0.43& $-0.004==pm$ 0.022& $-0.003$ ====
 0.090&  0.44& $ 0.008==pm$ 0.021& $-0.002$ ====
 0.101&  0.45& $ 0.038==pm$ 0.020& $-0.002$ ====
 0.113&  0.47& $-0.002==pm$ 0.019& $-0.002$ ====
 0.128&  0.48& $-0.017==pm$ 0.019& $-0.002$ ====
 0.144&  0.49& $-0.004==pm$ 0.019& $-0.002$ ====
 0.162&  0.50& $ 0.015==pm$ 0.019& $-0.002$ ====
 0.182&  0.51& $ 0.028==pm$ 0.019& $-0.002$ ====
 0.205&  0.52& $ 0.012==pm$ 0.020& $-0.005$ ====
 0.231&  0.53& $ 0.016==pm$ 0.021& $-0.003$ ====
 0.259&  0.53& $ 0.009==pm$ 0.022& $ 0.005$ ====
 0.292&  0.54& $ 0.028==pm$ 0.024& $ 0.005$ ====
 0.329&  0.55& $ 0.031==pm$ 0.026& $-0.004$ ====
 0.370&  0.55& $-0.032==pm$ 0.027& $-0.009$ ====
 0.417&  0.56& $ 0.029==pm$ 0.030& $-0.014$ ====
 0.469&  0.56& $-0.039==pm$ 0.032& $-0.019$ ====
 0.527&  0.57& $-0.005==pm$ 0.045& $-0.029$ ====
 0.594&  0.57& $-0.008==pm$ 0.074& $-0.036$ ====
 0.669&  0.57& $-0.021==pm$ 0.110& $-0.039$ ====
 0.753&  0.58& $ 0.001==pm$ 0.117& $-0.042$ ====
 0.847&  0.58& $ 0.010==pm$ 0.142& $-0.046$ ====
 ==hline
==multicolumn{4}{c}{$==theta=7.0^==circ$} ====
==hline
 0.063&  0.60& $ 0.116==pm$ 0.133& $-0.005$ ====
 0.071&  0.64& $-0.036==pm$ 0.054& $-0.005$ ====
 0.080&  0.69& $ 0.013==pm$ 0.037& $-0.004$ ====
 0.090&  0.74& $-0.013==pm$ 0.028& $-0.003$ ====
 0.101&  0.78& $ 0.016==pm$ 0.024& $-0.003$ ====
 0.113&  0.82& $ 0.024==pm$ 0.022& $-0.003$ ====
 0.128&  0.86& $ 0.052==pm$ 0.021& $-0.002$ ====
 0.144&  0.90& $ 0.012==pm$ 0.020& $-0.002$ ====
 0.162&  0.93& $ 0.036==pm$ 0.020& $-0.001$ ====
 0.182&  0.97& $ 0.027==pm$ 0.019& $-0.001$ ====
 0.205&  1.00& $ 0.005==pm$ 0.019& $ 0.000$ ====
 0.231&  1.03& $ 0.044==pm$ 0.019& $ 0.000$ ====
 0.259&  1.06& $ 0.019==pm$ 0.020& $ 0.001$ ====
 0.292&  1.09& $ 0.021==pm$ 0.020& $ 0.002$ ====
 0.329&  1.12& $ 0.034==pm$ 0.021& $ 0.002$ ====
 0.370&  1.14& $ 0.036==pm$ 0.022& $-0.003$ ====
 0.417&  1.16& $ 0.068==pm$ 0.023& $-0.001$ ====
 0.469&  1.19& $ 0.020==pm$ 0.025& $ 0.007$ ====
 0.527&  1.21& $ 0.024==pm$ 0.029& $ 0.001$ ====
 0.594&  1.22& $ 0.022==pm$ 0.033& $-0.011$ ====
 0.669&  1.24& $ 0.028==pm$ 0.039& $-0.029$ ====
 0.753&  1.25& $ 0.000==pm$ 0.068& $-0.054$ ====
 0.847&  1.26& $-0.018==pm$ 0.118& $-0.066$ ====
==end{tabular}
 ==end{table}
 ==end{document}