\documentstyle[12pt]{article}
\textwidth=165mm
\textheight=234mm
\topmargin=-15mm
\baselineskip=7.mm

\begin{document}
\newcommand{\vv}{\vspace{-0.5mm}}
\newcommand{\va}{\hspace*{5.mm}}
\newcommand{\vb}{\hspace*{2.mm}}
\newcommand{\vc}{\hspace*{3.8mm}}
\newcommand{\vd}{\hspace*{2.mm}}
\newcommand{\ha}{\hspace*{5.1mm}}

\begin{center}
Table 1 \,\, Atmospheric parameters for the non-thermal flare model 

\vspace{2.mm}
\begin{tabular}{rcrccc}
\hline \hline
$h$\va & $m-m_{0}$ & $T$\vc & $V_{t}$ &$N_{H}$ &$N_{e}$\\
(km)\vb & (g cm$^{-2}$) & (K)\vd & (km s$^{-1}$) & (cm$^{-3}$) & (cm$^{-3}$)\\
\hline
\vv
  1122.45 & 4.170E$-$06 & 150000 & 8.81 & 1.412E+12 & 1.699E+12 \\ \vv
  1119.74 & 5.360E$-$06 &  90000 & 8.78 & 2.326E+12 & 2.798E+12 \\ \vv
  1119.03 & 5.960E$-$06 &  40000 & 8.74 & 5.046E+12 & 6.068E+12 \\ \vv
  1118.30 & 6.960E$-$06 &  29000 & 8.70 & 6.912E+12 & 8.027E+12 \\ \vv
  1117.57 & 8.360E$-$06 &  20000 & 8.33 & 9.978E+12 & 1.098E+13 \\ \vv
  1116.89 & 1.012E$-$05 &  17000 & 7.62 & 1.178E+13 & 1.294E+13 \\ \vv
  1116.55 & 1.117E$-$05 &  14500 & 6.58 & 1.417E+13 & 1.521E+13 \\ \vv
  1116.17 & 1.252E$-$05 &  12000 & 6.32 & 1.761E+13 & 1.726E+13 \\ \vv
  1115.93 & 1.361E$-$05 &   9970 & 5.95 & 2.238E+13 & 1.875E+13 \\ \vv
  1115.86 & 1.400E$-$05 &   9600 & 5.70 & 2.406E+13 & 1.882E+13 \\ \vv
  1115.80 & 1.436E$-$05 &   9240 & 5.61 & 2.579E+13 & 1.851E+13 \\ \vv
  1115.66 & 1.525E$-$05 &   8840 & 5.51 & 2.904E+13 & 1.655E+13 \\ \vv
  1115.55 & 1.600E$-$05 &   8580 & 5.25 & 3.295E+13 & 1.360E+13 \\ \vv
  1115.47 & 1.666E$-$05 &   8390 & 5.05 & 3.686E+13 & 1.031E+13 \\ \vv
  1093.38 & 2.219E$-$04 &   8210 & 4.74 & 4.274E+13 & 1.024E+13 \\ \vv
  1071.12 & 4.640E$-$04 &   8040 & 4.45 & 4.978E+13 & 9.627E+12 \\ \vv
  1048.92 & 7.440E$-$04 &   7870 & 4.28 & 5.755E+13 & 8.940E+12 \\ \vv
  1029.61 & 1.023E$-$03 &   7730 & 4.00 & 6.601E+13 & 8.426E+12 \\ \vv
   990.48 & 1.716E$-$03 &   7510 & 3.60 & 8.516E+13 & 7.773E+12 \\ \vv
   904.86 & 3.983E$-$03 &   7180 & 3.20 & 1.433E+14 & 6.888E+12 \\ \vv
   803.61 & 8.844E$-$03 &   6730 & 2.80 & 2.767E+14 & 5.616E+12 \\ \vv
   729.98 & 1.510E$-$02 &   6410 & 2.55 & 4.577E+14 & 4.812E+12 \\ \vv
   664.06 & 2.411E$-$02 &   6170 & 2.44 & 7.229E+14 & 4.248E+12 \\ \vv
   565.36 & 4.874E$-$02 &   5890 & 2.14 & 1.480E+15 & 3.665E+12 \\ \vv
   506.03 & 7.500E$-$02 &   5705 & 1.80 & 2.348E+15 & 3.349E+12 \\ \vv
   465.43 & 1.014E$-$01 &   5550 & 1.70 & 3.247E+15 & 3.094E+12 \\ \vv
   417.50 & 1.461E$-$01 &   5422 & 1.50 & 4.792E+15 & 2.961E+12 \\ \vv
   394.24 & 1.750E$-$01 &   5350 & 1.30 & 5.844E+15 & 2.902E+12 \\ \vv
   374.22 & 2.050E$-$01 &   5275 & 1.10 & 6.975E+15 & 2.844E+12 \\ \vv
   336.89 & 2.772E$-$01 &   5190 & 1.02 & 9.577E+15 & 2.860E+12 \\ \vv
   314.16 & 3.336E$-$01 &   5130 & 0.99 & 1.165E+16 & 2.886E+12 \\ \vv
   262.61 & 5.105E$-$01 &   5100 & 0.88 & 1.794E+16 & 3.274E+12 \\ \vv
   186.43 & 9.607E$-$01 &   5140 & 0.84 & 3.346E+16 & 4.659E+12 \\ \vv
   135.75 & 1.451E$+$00 &   5210 & 0.80 & 4.987E+16 & 6.443E+12 \\ \vv
   104.21 & 1.868E$+$00 &   5295 & 0.78 & 6.319E+16 & 8.229E+12 \\ \vv
    78.54 & 2.286E$+$00 &   5395 & 0.82 & 7.582E+16 & 1.032E+13 \\ \vv
    62.82 & 2.580E$+$00 &   5510 & 0.87 & 8.369E+16 & 1.243E+13 \\ \vv
    39.79 & 3.067E$+$00 &   5660 & 0.95 & 9.668E+16 & 1.639E+13 \\ \vv
    16.67 & 3.630E$+$00 &   5805 & 1.10 & 1.111E+17 & 2.191E+13 \\ \vv
  $-$7.08 & 4.296E$+$00 &   5940 & 1.25 & 1.280E+17 & 2.952E+13 \\ \vv
 $-$18.22 & 4.640E$+$00 &   6050 & 1.35 & 1.353E+17 & 3.634E+13 \\ \vv
 $-$31.51 & 5.076E$+$00 &   6170 & 1.45 & 1.447E+17 & 4.621E+13 \\ \vv
 $-$50.35 & 5.750E$+$00 &   6310 & 1.55 & 1.598E+17 & 6.244E+13 \\ \vv
 $-$72.83 & 6.641E$+$00 &   6500 & 1.60 & 1.789E+17 & 9.262E+13 \\
$-$109.00 & 8.300E$+$00 &   6840 & 1.65 & 2.124E+17 & 1.805E+14 \\
\hline
\end{tabular}
\end{center}

\vspace{-2.5mm}
\hspace*{18.mm}$m_{0}=2.5\times 10^{-3}$

\newpage
\begin{center}
Table 2 \,\, Atmospheric parameters for the thermal flare model 

\vspace{2.mm}
\begin{tabular}{rcrccc}
\hline \hline
$h$\va & $m-m_{0}$ & $T$\vc & $V_{t}$ &$N_{H}$ &$N_{e}$\\
(km)\vb & (g cm$^{-2}$) & (K)\vd & (km s$^{-1}$) & (cm$^{-3}$) & (cm$^{-3}$)\\
\hline
\vv
  1108.52 & 4.170E$-$06 & 150000 & 8.81 & 1.807E+12 & 2.174E+12 \\ \vv
  1106.40 & 5.360E$-$06 &  90000 & 8.78 & 2.975E+12 & 3.579E+12 \\ \vv
  1105.84 & 5.960E$-$06 &  40000 & 8.74 & 6.456E+12 & 7.763E+12 \\ \vv
  1105.27 & 6.960E$-$06 &  29000 & 8.70 & 8.863E+12 & 1.024E+13 \\ \vv
  1104.71 & 8.360E$-$06 &  20000 & 8.33 & 1.276E+13 & 1.405E+13 \\ \vv
  1104.17 & 1.012E$-$05 &  17000 & 7.62 & 1.506E+13 & 1.655E+13 \\ \vv
  1103.90 & 1.117E$-$05 &  14500 & 6.58 & 1.815E+13 & 1.940E+13 \\ \vv
  1103.61 & 1.252E$-$05 &  12000 & 6.32 & 2.252E+13 & 2.201E+13 \\ \vv
  1103.42 & 1.361E$-$05 &   9973 & 5.95 & 2.859E+13 & 2.405E+13 \\ \vv
  1103.37 & 1.400E$-$05 &   9617 & 5.70 & 3.074E+13 & 2.387E+13 \\ \vv
  1103.32 & 1.436E$-$05 &   9250 & 5.61 & 3.302E+13 & 2.318E+13 \\ \vv
  1103.21 & 1.525E$-$05 &   8885 & 5.51 & 3.725E+13 & 1.993E+13 \\ \vv
  1103.13 & 1.600E$-$05 &   8640 & 5.25 & 4.206E+13 & 1.646E+13 \\ \vv
  1102.13 & 2.666E$-$05 &   8450 & 5.05 & 4.684E+13 & 1.223E+13 \\ \vv
  1085.28 & 2.219E$-$04 &   8300 & 4.74 & 5.258E+13 & 1.181E+13 \\ \vv
  1066.86 & 4.640E$-$04 &   8180 & 4.45 & 5.949E+13 & 1.110E+13 \\ \vv
  1047.92 & 7.440E$-$04 &   8090 & 4.28 & 6.639E+13 & 1.061E+13 \\ \vv
  1030.96 & 1.023E$-$03 &   8010 & 4.00 & 7.408E+13 & 1.023E+13 \\ \vv
   995.38 & 1.716E$-$03 &   7880 & 3.60 & 9.173E+13 & 9.768E+12 \\ \vv
   914.38 & 3.983E$-$03 &   7540 & 3.20 & 1.489E+14 & 7.812E+12 \\ \vv
   814.89 & 8.844E$-$03 &   7080 & 2.80 & 2.782E+14 & 5.421E+12 \\ \vv
   740.69 & 1.510E$-$02 &   6760 & 2.55 & 4.512E+14 & 4.127E+12 \\ \vv
   673.75 & 2.411E$-$02 &   6430 & 2.44 & 7.129E+14 & 2.965E+12 \\ \vv
   573.75 & 4.874E$-$02 &   6030 & 2.14 & 1.467E+15 & 2.111E+12 \\ \vv
   513.83 & 7.500E$-$02 &   5830 & 1.80 & 2.320E+15 & 1.870E+12 \\ \vv
   472.70 & 1.014E$-$01 &   5680 & 1.70 & 3.197E+15 & 1.702E+12 \\ \vv
   424.00 & 1.461E$-$01 &   5520 & 1.50 & 4.731E+15 & 1.619E+12 \\ \vv
   400.44 & 1.750E$-$01 &   5450 & 1.30 & 5.762E+15 & 1.632E+12 \\ \vv
   380.16 & 2.050E$-$01 &   5350 & 1.10 & 6.902E+15 & 1.579E+12 \\ \vv
   342.44 & 2.772E$-$01 &   5255 & 1.02 & 9.484E+15 & 1.740E+12 \\ \vv
   319.52 & 3.336E$-$01 &   5180 & 0.99 & 1.156E+16 & 1.857E+12 \\ \vv
   267.70 & 5.105E$-$01 &   5120 & 0.88 & 1.790E+16 & 2.480E+12 \\ \vv
   191.37 & 9.607E$-$01 &   5150 & 0.84 & 3.342E+16 & 4.235E+12 \\ \vv
   140.70 & 1.451E$+$00 &   5210 & 0.80 & 4.990E+16 & 6.178E+12 \\ \vv
   109.16 & 1.868E$+$00 &   5295 & 0.78 & 6.321E+16 & 8.048E+12 \\ \vv
    83.50 & 2.286E$+$00 &   5395 & 0.82 & 7.585E+16 & 1.020E+13 \\ \vv
    67.78 & 2.580E$+$00 &   5510 & 0.87 & 8.372E+16 & 1.234E+13 \\ \vv
    44.76 & 3.067E$+$00 &   5660 & 0.95 & 9.670E+16 & 1.634E+13 \\ \vv
    21.64 & 3.630E$+$00 &   5805 & 1.10 & 1.112E+17 & 2.191E+13 \\ \vv
  $-$2.11 & 4.296E$+$00 &   5940 & 1.25 & 1.280E+17 & 2.955E+13 \\ \vv
 $-$13.25 & 4.640E$+$00 &   6050 & 1.35 & 1.353E+17 & 3.639E+13 \\ \vv
 $-$26.52 & 5.076E$+$00 &   6160 & 1.45 & 1.450E+17 & 4.561E+13 \\ \vv
 $-$45.36 & 5.750E$+$00 &   6310 & 1.55 & 1.598E+17 & 6.258E+13 \\ \vv
 $-$67.83 & 6.641E$+$00 &   6500 & 1.60 & 1.790E+17 & 9.284E+13 \\
$-$104.00 & 8.300E$+$00 &   6840 & 1.65 & 2.124E+17 & 1.809E+14 \\
\hline
\end{tabular}
\end{center}

\vspace{-2.5mm}
\hspace*{18.mm}$m_{0}=3.2\times 10^{-3}$

\newpage
\begin{center}
Table 3 \,\, Atmospheric parameters for the pre-flare model 

\vspace{2.mm}
\begin{tabular}{rcrccc}
\hline \hline
$h$\va & $m-m_{0}$ & $T$\vc & $V_{t}$ &$N_{H}$ &$N_{e}$\\
(km)\vb & (g cm$^{-2}$) & (K)\vd & (km s$^{-1}$) & (cm$^{-3}$) & (cm$^{-3}$)\\
\hline
\vv
  1364.85 & 5.750E$-$07 & 141000 & 9.87 & 1.565E+11 & 1.883E+11 \\ \vv
  1358.39 & 8.680E$-$07 &  90000 & 9.76 & 2.424E+11 & 2.915E+11 \\ \vv
  1357.10 & 9.510E$-$07 &  70000 & 9.73 & 3.085E+11 & 3.711E+11 \\ \vv
  1355.80 & 1.082E$-$06 &  38000 & 9.33 & 5.505E+11 & 6.619E+11 \\ \vv
  1354.45 & 1.292E$-$06 &  26000 & 8.78 & 8.057E+11 & 9.214E+11 \\ \vv
  1352.78 & 1.642E$-$06 &  20430 & 8.74 & 1.023E+12 & 1.113E+12 \\ \vv
  1352.09 & 1.825E$-$06 &  16100 & 8.71 & 1.265E+12 & 1.357E+12 \\ \vv
  1351.18 & 2.126E$-$06 &  12700 & 7.63 & 1.652E+12 & 1.663E+12 \\ \vv
  1350.98 & 2.210E$-$06 &  11700 & 7.40 & 1.838E+12 & 1.727E+12 \\ \vv
  1350.76 & 2.313E$-$06 &   9900 & 7.28 & 2.338E+12 & 1.644E+12 \\ \vv
  1350.57 & 2.430E$-$06 &   9100 & 7.00 & 2.768E+12 & 1.420E+12 \\ \vv
  1350.38 & 2.557E$-$06 &   8570 & 6.70 & 3.073E+12 & 1.187E+12 \\ \vv
  1340.47 & 1.025E$-$05 &   8395 & 6.38 & 3.548E+12 & 1.034E+12 \\ \vv
  1316.47 & 3.225E$-$05 &   8190 & 5.65 & 4.220E+12 & 1.047E+12 \\ \vv
  1257.36 & 1.008E$-$04 &   7860 & 5.26 & 5.803E+12 & 9.897E+11 \\ \vv
  1211.58 & 1.730E$-$04 &   7580 & 4.88 & 7.653E+12 & 8.757E+11 \\ \vv
  1175.41 & 2.455E$-$04 &   7390 & 4.70 & 9.451E+12 & 7.955E+11 \\ \vv
  1115.39 & 4.060E$-$04 &   7107 & 4.51 & 1.336E+13 & 6.803E+11 \\ \vv
  1070.65 & 5.674E$-$04 &   6910 & 4.35 & 1.741E+13 & 6.023E+11 \\ \vv
   909.31 & 1.738E$-$03 &   6286 & 3.20 & 5.066E+13 & 4.170E+11 \\ \vv
   772.95 & 4.643E$-$03 &   5783 & 2.04 & 1.448E+14 & 3.094E+11 \\ \vv
   679.64 & 9.423E$-$03 &   5380 & 1.80 & 3.103E+14 & 2.196E+11 \\ \vv
   589.19 & 1.965E$-$02 &   4970 & 1.62 & 6.946E+14 & 1.675E+11 \\ \vv
   504.72 & 4.273E$-$02 &   4610 & 1.30 & 1.637E+15 & 2.151E+11 \\ \vv
   454.60 & 6.900E$-$02 &   4328 & 1.02 & 2.835E+15 & 2.781E+11 \\ \vv
   419.65 & 9.715E$-$02 &   4285 & 0.96 & 4.036E+15 & 3.552E+11 \\ \vv
   332.65 & 2.290E$-$01 &   4345 & 0.86 & 9.399E+15 & 7.404E+11 \\ \vv
   228.73 & 6.174E$-$01 &   4535 & 0.70 & 2.438E+16 & 1.921E+12 \\ \vv
   181.37 & 9.600E$-$01 &   4605 & 0.68 & 3.734E+16 & 2.881E+12 \\ \vv
   155.81 & 1.210E$+$00 &   4680 & 0.65 & 4.635E+16 & 3.685E+12 \\ \vv
   135.52 & 1.451E$+$00 &   4736 & 0.60 & 5.498E+16 & 4.453E+12 \\ \vv
   120.29 & 1.660E$+$00 &   4794 & 0.62 & 6.212E+16 & 5.185E+12 \\ \vv
   106.77 & 1.868E$+$00 &   4844 & 0.66 & 6.913E+16 & 5.912E+12 \\ \vv
    93.96 & 2.086E$+$00 &   4914 & 0.70 & 7.604E+16 & 6.794E+12 \\ \vv
    83.20 & 2.286E$+$00 &   4960 & 0.70 & 8.256E+16 & 7.554E+12 \\ \vv
    68.75 & 2.580E$+$00 &   5060 & 0.78 & 9.118E+16 & 8.900E+12 \\ \vv
    57.94 & 2.820E$+$00 &   5127 & 0.82 & 9.828E+16 & 9.989E+12 \\ \vv
    47.57 & 3.067E$+$00 &   5217 & 0.86 & 1.050E+17 & 1.133E+13 \\ \vv
    36.47 & 3.350E$+$00 &   5310 & 0.90 & 1.125E+17 & 1.293E+13 \\ \vv
    26.19 & 3.630E$+$00 &   5402 & 0.95 & 1.197E+17 & 1.469E+13 \\ \vv
    14.82 & 3.960E$+$00 &   5510 & 1.00 & 1.279E+17 & 1.710E+13 \\ \vv
 $-$12.90 & 4.860E$+$00 &   5795 & 1.20 & 1.485E+17 & 2.646E+13 \\ \vv
 $-$36.92 & 5.750E$+$00 &   6095 & 1.36 & 1.663E+17 & 4.434E+13 \\ \vv
 $-$58.62 & 6.641E$+$00 &   6350 & 1.50 & 1.837E+17 & 7.215E+13 \\
 $-$94.00 & 8.300E$+$00 &   6720 & 1.60 & 2.164E+17 & 1.484E+14 \\
\hline
\end{tabular}
\end{center}

\vspace{-2.5mm}
\hspace*{18.mm}$m_{0}=2.62\times 10^{-4}$
\end{document}