\documentstyle[12pt,aasms]{article} % \setlength{\textwidth}{11.0in} \setlength{\textheight}{8.5in} \setlength{\topmargin}{0.0in} \setlength{\oddsidemargin}{-1.0in} \setlength{\evensidemargin}{\oddsidemargin} % \font\tenrm = cmr10 \setcounter{page}{15} \setcounter{table}{6} \pagestyle{plain} \begin{document} \begin{table*} \caption{{\sc Rotationless Dipole Moments, ${\cal M}^{v}_{v}(0)$, for the Pure Rotational Transitions (D)}} {\tenrm \begin{center} \begin{tabular}{rrrrrrrr} \tableline \tableline \multicolumn{1}{c}{v} & \multicolumn{1}{c}{$^{12}$C$^{16}$O} & \multicolumn{1}{c}{$^{13}$C$^{16}$O} & \multicolumn{1}{c}{$^{12}$C$^{18}$O} & \multicolumn{1}{c}{$^{12}$C$^{17}$O} & \multicolumn{1}{c}{$^{13}$C$^{18}$O} & \multicolumn{1}{c}{$^{14}$C$^{16}$O} & \multicolumn{1}{c}{$^{13}$C$^{17}$O} \\ \tableline 0&$-$1.1013($-$01)& $-$1.1046($-$01)&$-$1.1049($-$01)&$-$1.1034($-$01)&$-$1.1079($-$01)&$-$1.1072($-$01)&$-$1.1063($-$01) \\ 1&$-$8.5066($-$02)& $-$8.5962($-$02)&$-$8.6034($-$02)&$-$8.5598($-$02)&$-$8.6906($-$02)&$-$8.6705($-$02)&$-$8.6460($-$02) \\ 2&$-$5.9961($-$02)& $-$6.1420($-$02)&$-$6.1539($-$02)&$-$6.0815($-$02)&$-$6.2987($-$02)&$-$6.2652($-$02)&$-$6.2246($-$02) \\ 3&$-$3.4803($-$02)& $-$3.6824($-$02)&$-$3.6990($-$02)&$-$3.5977($-$02)&$-$3.9017($-$02)&$-$3.8549($-$02)&$-$3.7980($-$02) \\ 4&$-$9.5731($-$03)& $-$1.2160($-$02)&$-$1.2374($-$02)&$-$1.1070($-$02)&$-$1.4984($-$02)&$-$1.4381($-$02)&$-$1.3650($-$02) \\ 5& 1.5743($-$02)& 1.2583($-$02)& 1.2322($-$02)& 1.3919($-$02)& 9.1241($-$03)& 9.8620($-$03)& 1.0759($-$02) \\ \tableline \end{tabular} \end{center} }% \vspace{3.0in} \centerline{\thepage} \end{table*} \end{document}