\begin{table}%t2 \caption{\label{tabcomp}Conal emission geometry parameters of PSRs B1839+09, B1916+14 and B2111+46.} %\bigskip \smallskip %\centerline {\small \begin{tabular}{ccrrrrrrccrrr} \hline \hline \multicolumn{1}{c}{Pulsar} & \multicolumn{1}{c}{$\nu$} & \multicolumn{1}{c}{Cone} &\multicolumn{1}{c}{$\phi'_{\rm L}$} & \multicolumn{1}{c}{$\phi'_{\rm T}$} & \multicolumn{1}{c}{$\delta\phi'$} &\multicolumn{1}{c} {$\Gamma$} &\multicolumn{1}{c}{$r$} &\multicolumn{1}{c}{$r$} & \multicolumn{1}{c}{$s/s_{\rm lof}$} \\ \multicolumn{1}{c}{PSR B} & \multicolumn{1}{c}{(MHz)} & \multicolumn{1}{c}{(No.)} & \multicolumn{1}{c}{($^\circ$)} & \multicolumn{1}{c}{($^\circ$)} & \multicolumn{1}{c} {($^\circ$)} &\multicolumn{1}{c} {($^\circ$)} & \multicolumn{1}{c}{(km)\tablefootmark{a}} &\multicolumn{1}{c}{$(\%~~ r_{\rm LC}$)} & \multicolumn{1}{c}{foot value} \\ \multicolumn{1}{c}{(1)} & \multicolumn{1}{c}{(2)} & \multicolumn{1}{c}{(3)} & \multicolumn{1}{c}{(4)} & \multicolumn{1}{c}{(5)} & \multicolumn{1}{c}{(6)} & \multicolumn{1}{c}{(7)} & \multicolumn{1}{c}{(8)} & \multicolumn{1}{c}{(9)} & \multicolumn{1}{c}{(10)} \\ \hline 1839+09 & 1418&1 & $-3.75\pm0.15$ & $2.96\pm0.18$ & $-0.39\pm0.12$ & $4.06\pm2.30$ & $63\pm19$ & $0.34\pm0.10$ & $ 0.80\pm0.10$\\ 1916+14 & 1418&1 & $-3.49\pm0.05$ & $2.04\pm0.07$ & $-0.72\pm0.04$ & $2.63\pm1.00$ & $299\pm18$ & $0.63\pm0.04$ & $ 0.39\pm0.01$\\ 2111+46 & 610&1 & $-14.78\pm0.45$ & $11.79\pm0.31$ & $-1.49\pm0.27$ & $2.85\pm 1.10$ & $581\pm107$ & $ 1.20\pm0.22$ & $ 0.30\pm0.02$\\ & &2 & $-33.83\pm0.21$ & $24.95\pm0.22$ & $-4.44\pm0.15$ & $5.87\pm1.10$ & $1891\pm64$ & $3.91\pm0.13$ & $ 0.35\pm0.00$\\ & 1408&1 & $-14.70\pm0.40$ & $11.78\pm0.34$ & $-1.46\pm0.27$ & $3.30\pm1.80$ & $533\pm97$ & $1.10\pm0.20$ & $ 0.37\pm0.03$\\ & &2 & $-28.47\pm0.31$ & $22.48\pm0.34$ & $-2.99\pm0.23$ & $5.58\pm1.80$ & $1151\pm 87$ & $2.38\pm0.18$ & $ 0.42\pm0.01$\\ \hline \end{tabular}} \tablefoot{\tablefoottext{a}{Emission heights computed using the exact formula (G05).}} \end{table}