\begin{table}%t4 \caption{\label{ta:noclump}Positions (J2000) and determined properties toward the positions without clumps.} %\centering \par \begin{tabular}{l l r r r r r r r } \hline\hline \noalign{\smallskip} HEC name & & \multicolumn{1}{c}{RA} & \multicolumn{1}{c}{Declination} & \multicolumn{1}{c}{$d_{\rm kin}$} &\multicolumn{1}{c}{$F^i_{{\rm 0.25 pc}}$}&\multicolumn{1}{c}{$M_{0.25~{\rm pc}}$} &\multicolumn{1}{c}{$T_{{\rm rot}}$} &\multicolumn{1}{c}{${N_{{\rm NH_3}}}$} \\ & & \multicolumn{1}{c}{(h:m:s)} & \multicolumn{1}{c}{(\degr:~\arcmin:~\arcsec)} &(kpc)&(mJy)& \multicolumn{1}{c}{(${M_\odot}$)} &\multicolumn{1}{c}{(K)} & \multicolumn{1}{c}{($10^{15}$~cm$^{-2}$)}\\ \hline G012.73--00.58... &MM2 & 18:15:32.7 & --18:10:15 & 1.1&178 &8 & 11.4(0.7) & .. \\ G013.97--00.45... &MM1 & 18:17:16.5 & --17:01:16 & 2.4&189 &25 & 16.6(0.9) & .. \\ G014.39--00.75A.. &MM2 & 18:19:17.4 & --16:44:04 & 2.1&382 &32 & 20.0(2.3) & .. \\ G023.38--00.12... &MM2 & 18:34:20.4 & --8:33:16 & 5.6&.. & 44 &17.8(2.0). &.. \\ G025.79+00.81... &MM1 & 18:35:20.5 & --5:56:36 & 3.4 &196 & 77 & 13.1(0.7) & .. \\ &MM2 & 18:35:26.3 & --5:59:21 & 3.4 & 63 & 31 & .. &..\\ G034.03--00.33... &MM1 & 18:54:25.1 & 0:49:56 & .. &.. & .. & .. &.. \\ &2 & 18:54:39.2 & 0:51:37 & .. &.. & .. & .. & .. \\ G034.34--00.90... &1 & 18:57:16.5 & 0:50:48 &.. &.. &.. &..\\ G034.77--00.81... &MM1 & 18:57:40.7 & 1:16:09 & 2.9 & 49 & 11 & .. & ..\\ G034.85+00.43... &MM1 & 18:53:23.2 & 1:53:16 &3.6 & 73 & 31 &13.2(1.5) & ..\\ G037.44+00.14A.. &MM1 & 18:59:14.0 & 4:07:37 &1.3 & 163 & 8 & .. &.. \\ G037.44+00.14B.. &MM2 & 18:59:10.2 & 4:04:32 &1.7 & 130 & .. & .. &..\\ \hline \end{tabular} \tablefoot {The first two columns give the HEC name and the millimeter clump number, the following columns represent (in order of appearance): right ascension, declination, kinematic distance, integrated 1.2~mm flux within 0.25~pc diameter, mass within 0.25~pc diameter, \amm\ rotational temperature, and \amm\ column density.} %\vspace*{5mm} \end{table}