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{
\begin{planotable}{llllllll}
\tablenum{3(a)}
\tablewidth{9.0in}
\tablecaption{ADOPTED X-RAY POWER LAW FITS}
\tablehead{
\colhead{Object} &
\colhead{0.2 keV } &
\colhead{1 keV } &
\colhead{1 keV } &
\colhead{Ref} &
\colhead{4 keV } &
\colhead{4 keV } &
\colhead{Ref}  \\[.2ex]
\colhead{} &
\colhead{flux ($\mu$Jy)} &
\colhead{Energy index} &
\colhead{flux ($\mu$Jy)} &
\colhead{} &
\colhead{Energy index} &
\colhead{flux ($\mu$Jy)} &
\colhead{} 
}
\startdata
Q0003+158 &
& 2.2\er$^{2.8}_{1.3}$ & 1.40\er$^{6.0}_{0.6}$ & 1 &  & $<$1.5 & 9\\
Q0003+199 &   & 2.0 & 6.5--8.5 & 10 & 1.0 & 0.8--1.1 & 10\\ 
Q0007+106 &
& 0.4\er$^{0.9}_{0.3}$&1.97\er$^{2.49}_{0.52}$ & 2&0.66
\er$^{0.09}_{0.14}$&2.08&6\\
Q0026+129 & 5.9\er$^{1.4}_{1.1}$
&0.88\er$^{0.05}_{0.05}$ & 1.41\er$^{0.03}_{0.03}$ & 3 &
0.86\er$^{0.39}_{0.38}$&0.43&5\\
Q0049+171&   
&1.2\er$^{  2.8      }_{  0.6     }$ &   2.58\er$^{  5.95     }_{   0.67     }$&1&
1.03\er$^{0.29}_{0.29}$&0.57&5\\
Q0050+124&
&  1.9\er$^{1.7}_{0.8}$ & 3.60\er$^{6.7}_{1.3}$ &1 & & $<$1.1 & 9\\
Q0052+251&  
&  1.2\er$^{  1.7  }_{  0.6      }$ &   1.63\er$^{   3.5     }_{   0.5     }$&1
&0.84\er$^{0.53}_{0.53}$&0.28&5\\
Q0054+144
&5.18\er$^{1.6}_{1.6}$
 & 0.41\er$^{0.07}_{0.07}$       & 0.52\er$^{0.04}_{0.04}$ & 3&
0.07\er$^{0.67}_{0.64}$&0.23&12\\ 
Q0121$-$590&  
&  0.9\er$^{  0.2      }_{  0.1      }$ &   9.04\er$^{   0.72     }_{   0.60     }$
&1&1.07\er$^{0.07}_{0.07}$&0.91&6\\
Q0134+329
& &0.7\er$^{0.4}_{0.4}$ & 0.50\er$^{0.14}_{0.10}$&2&&&\\
Q0205+024&18.8\er$^{4.5}_{5.0}$ 
& 1.2\er$^{0.07}_{0.07}$ & 0.58\er$^{0.06}_{0.06}$ & 3&&&\\
Q0312$-$770&
& 0.1\er$^{0.6}_{0.2}$ & 0.49\er$^{0.59}_{0.09}$ & 2&&&\\
Q0414-060 &   & 0.5\er$^{1.7}_{0.3}$ & 0.32\er$^{0.8}_{0.1}$ & 1\\
Q0637$-$752&$<$34.8 
& 0.46\er$^{0.10}_{0.10}$ & 0.98\er$^{0.05}_{0.05}$& 3&
0.93\er$^{0.64}_{0.60}$&0.31&5\\
&& & & &
0.83\er$^{0.15}_{0.08}$&0.59&7\\
Q0804+761&    
&  1.01\er$^{0.51}_{0.45}$ & 2.00\er$^{0.46}_{0.41}$ & 1& 
1.08\er$^{0.16}_{0.11}$&0.38&7\\
Q0837$-$120&    
&  0.65\er$^{  0.27      }_{  0.23      }$ &   1.74\er$^{   0.31     }_{   0.19     }$&1&
0.89\er$^{0.28}_{0.17}$&0.36&7\\
Q0844+349  &
&  0.53\er$^{  0.62      }_{  0.34      }$ &   0.49\er$^{   0.13     }_{   0.03    }$&1&&
$<$1.8&9\\
Q0915+165 &   & 0.3\er$^{0.3}_{0.2}$ & 1.28\er$^{0.16}_{0.09}$ & 1
          &   & 0.5 &9\\
Q0923+129 &   & 0.7\er$^{0.4}_{0.4}$ & 1.45\er$^{0.27}_{0.24}$ & 1\\
Q1028+313  &7.5\er$^{2.0}_{2.1}$ 
&  0.62\er$^{0.06}_{0.06}$ & 0.76\er$^{0.07}_{0.07}$ & 3&&&\\
Q1100+772
& & 1.0\er$^{0.3}_{0.5}$ & 0.69\er$^{0.19}_{0.13}$&2&&$<$5.7&9\\
Q1116+215
& & 1.0\er$^{0.3}_{0.2}$ & 0.68\er$^{0.12}_{0.06}$&2&&$<$1.7&9\\
Q1137+660&
&0.7\er$^{0.4}_{0.1}$& 0.39\er$^{0.08}_{0.02}$&2&&&\\
Q1146$-$037
&&0.3\er$^{0.5}_{0.2}$& 0.56\er$^{0.26}_{0.07}$&2&&&\\
Q1202+281
&&1.1\er$^{0.2}_{0.4}$& 1.19\er$^{0.27}_{0.25}$&2&&$<$1.6&9\\
Q1211+143
& &2.0\er$^{0.3}_{0.2}$& 5.5\er$^{0.8}_{0.7}$&4&
1.02\er$^{0.23}_{0.22}$&0.64&5\\
&&&&&
1.11\er$^{0.17}_{0.13}$&0.50&7\\
Q1219+755 
&16.7\er$^{2.4}_{2.5}$ & 0.78\er$^{0.03}_{0.03}$ & 2.24\er$^{0.08}_{0.08}$& 3&
1.17\er$^{0.67}_{0.60}$&0.45&5\\
&&&&&
0.91\er$^{0.09}_{0.09}$&0.57&7\\
Q1226+023
&48.9\er$^{3.3}_{3.3}$
  & 0.47\er$^{0.03}_{0.03}$ & 9.8\er$^{0.2}_{0.2}$&3&
0.53\er$^{0.03}_{0.03}$&5.05&5\\
&& & & &
0.44\er$^{0.02}_{0.02}$&5.84&7\\
Q1244+026 &   & 1.4\er$^{1.1}_{0.4}$ & 0.78\er$^{0.11}_{0.12}$ & 1
     &   & $<$1.2 & 9\\
Q1307+085 
&& 0.9\er$^{0.5}_{0.2}$&0.81\er$^{0.12}_{0.06}$ &2&
0.86\er$^{0.15}_{0.08}$&0.40&7\\
Q1351+695
&& 1.1\er$^{0.2}_{0.3}$ & 3.7\er$^{0.3}_{0.3}$ & 1\\
Q1352+183
&&1.5\er$^{0.7}_{0.6}$ &0.56\er$^{0.04}_{0.09}$ &1
&  & 0.10 & 7\\
Q1407+265
& & 1.2\er$^{0.9}_{0.2}$&0.44\er$^{0.17}_{0.05}$ & 2&&0.10&7\\
\tablebreak
Q1416$-$129
&& 0.9\er$^{0.5}_{0.5}$&2.15\er$^{3.50}_{0.70}$ & 2&
0.10\er$^{0.10}_{0.10}$&0.35&7\\
Q1426+015
& $<$50.4& 1.12\er$^{0.1}_{0.1}$ & 3.05\er$^{0.09}_{0.09}$ & 3 &
0.46\er$^{0.25}_{0.25}$&0.62&5\\
Q1501+106
&49.3\er$^{8.3}_{9.3}$ & 0.93\er$^{0.04}_{0.04}$ & 4.2\er$^{0.3}_{0.3}$ & 3&
0.42\er$^{0.16}_{0.16}$&1.04&5\\
Q1545+210 &
& 0.8\er$^{0.3}_{0.5}$ & 1.10\er$^{0.43}_{0.29}$&2&&$<$1.4&9\\
Q1613+658
&$<$20.3 & 1.10\er$^{0.2}_{0.3}$ & 1.40\er$^{0.04}_{0.04}$ & 3&&0.8\er$^{0.3}_{0.3}$&9\\
Q1635+119 &   & 0.7\er$^{1.7}_{0.6}$ & 0.35\er$^{0.83}_{0.09}$ & 1\\
Q1704+608
&  &  0.4\er$^{  0.6      }_{  0.4      }$ &   0.15\er$^{   0.06     }_{   0.03     }$&1&
&$<$1.4&9\\
Q1721+343
& & 0.5\er$^{0.4}_{0.3}$ & 1.93\er$^{0.73}_{0.20}$ & 2 &0.64\er$^{0.17}_{0.14}$&0.67&8\\
Q1803+676 &
& -0.2\er$^{0.4}_{0.3}$ & 0.33\er$^{0.20}_{0.06}$ & 2 &&&\\
Q2128-123 &   & 0.5\er$^{0.7}_{0.4}$ & 0.49\er$^{0.27}_{0.11}$ & 1\\
Q2130+099
&22.8\er$^{5.4}_{5.3}$ & 0.81\er$^{0.07}_{0.07}$ & 0.91\er$^{0.08}_{0.08}$ & 3&
1.27\er$^{0.36}_{0.36}$&0.36&5\\
&& & & &
1.29\er$^{0.19}_{0.16}$&0.31&7\\
Q2135$-$147 & $<$9.7
& 0.73\er$^{0.05}_{0.05}$ & 1.10\er$^{0.02}_{0.02}$ & 3&
0.83\er$^{0.33}_{0.31}$&0.57&5\\
&& & & &
0.86\er$^{0.08}_{0.08}$&0.78&7\\
Q2209+184 &   & 0.8\er$^{0.5}_{0.5}$ & 1.31\er$^{0.39}_{0.27}$ & 1\\
Q2251-178 &   & 0.4\er$^{0.6}_{0.6}$ & 3.30\er$^{2.3}_{1.3}$ & 1\\
\tablerefs{
1) This paper; 2) Wilkes and Elvis (1987); 3) Masnou et al (1992); 4) Elvis et al (1991);
5) Comastri et al (1992); 6) Turner and Pounds (1989); 7) Williams et al (1992);
8) Ohashi et al (1992); 9) Della Ceca et al (1990); 10) Turner and Pounds (1988);
11) Tananbaum et al (1986); 12) Saxton et al (1993).
}
\end{planotable}
}


{
\begin{planotable}{lllllllllll}
\tablenum{3(b)}
\tablewidth{9.0in}
\tablecaption{ OBSERVATIONAL DETAILS FOR NEW X-RAY POWER LAW FITS\tablenotemark{a}}
\tablehead{
\colhead{Object}&
\colhead{Sequence} &
\colhead{Date} &
\colhead{Exposure (s)} &
\colhead{Gain} &
\colhead{PHA Channels} &
\colhead{Fit Counts} &
\colhead{Count Rate} &
\colhead{$\alpha$} &
\colhead{$N_H$} &
\colhead{$\chi^2$} 
}
\startdata
Q0003+158 & 5360 & 1980 Jan 3 &2211 & 11.7 & 2:9 & 560 &0.11 &2.20  & 21.38 
& 9.9 \\
 && 1980 Jun 15 & 2955 & 16.0\\
Q0049+171 & 8431 & 1980 Jul 22 & 1373 & 15.5 & 2:10 & 488 & 0.36 & 1.16 & 20.94& 9.6 \\
Q0050+124 & 2632 & 1979 Jul 20 & 1552 & 14.6 & 2:10 & 555 & 0.36 & 1.85 & 21.18 & 6.7\\
Q0052+251 & 5334 & 1980 Jan 10 & 1472 & 16.4 & 2:11 & 351 & 0.24 & 1.16 & 20.90 & 8.7\\
Q0121-590 & 0523 & 1979 Nov 25 & 2566 & 12.6 & 1:9 & 5230 & 2.04 & 0.92 & 20.23 & 7.5\\
Q0414-060 & 0521 & 1979 Feb 25 & 4083 & 14.8 & 2:10 & 241  &0.06 & 0.48 & 20.65 & 1.8\\
Q0804+761 & 5336 & 1980 Sep 27 & 1303 & 14.1 & 2:10 & 465 & 0.36 & 1.01 & 20.49 & 10.2\\
Q0837-120 & 8933 & 1981 Apr 21 & 5367 & 16.2 &2:11 &1717 & 0.32 & 0.66 &  20.61 & 12.6  \\
Q0844+349 & 5337 & 1979 Oct 29 & 1659 & 18.7 & 2:12 & 1748 & 1.05 & 0.80 & 20.70 & 17.9\\
Q0915+165 & 3467 & 1979 Nov  6 & 1128 & 16.5 & 2:12 &904 &0.33  & 0.34 & 19.71 & 8.3 \\
 && 1979 Nov 13 & 1622 & 19.5\\
Q0923+129 & 6708 & 1980 May  7 & 2039 & 16.6 & 2:11 &610&0.30  & 0.70 & 20.35 & 6.5 \\
Q1244+026 & 8433 & 1980 Jul 13 & 1232 & 15.7 &2:10 &394 & 0.32& 1.40 &  19.75 & 8.0 \\
Q1351+695 & 10596 &1981 Feb  9 & 1547 & 18.3& 2:12 &1486 &0.96  & 1.06 &  20.20 & 12.6 \\
Q1352+183 & 5377 &  1981 Jan 11 & 2669 & 12.8 &1:9 & 418 & 0.16 & 1.54 &  20.30 & 3.0 \\
Q1704+608 & 5688 &1980 Jan 1-May 2&38084 & 16.6 & 2:11 & 1129 &0.03 & 0.43  & 20.47 & 6.6 \\
Q2128-123 & 8413 & 1980 May 9 & 5850 & 16.7 &2:11 &  531 &0.09& 0.52 &  20.60 & 3.3  \\
Q2209+184 & 8438 & 1980 Jun 15 & 1766 & 16.1 & 2:11 &  433&0.25 & 0.77 &  20.56 & 7.5  \\
Q2251-178 & 2074 & 1979 May 22 & 1958 & 11.8 & 1:9  &  994&0.51 & 0.37 &  21.20 & 12.6 \\
\tablenotetext{a}{For details of analysis, see Wilkes and Elvis (1987). For
normalizations and errors on fit parameters, see Table 3(a).}
\end{planotable}
}

\end{document}


