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Table 2:

Summary of the H I properties.
Object $v_{\rm0}$ (LSR) $I_{\rm H {\sc i}}$a $W_{\rm 50}$b LSc $M_{\rm H {\sc i}}$ $M_{\rm dyn}$ $M_{\rm tot, gas}$ $L^{\prime}$$_{\rm CO}$ /  $M_{\rm H {\sc i}}$ $L_{\rm IR}$ f $\Sigma$M $M_{\rm H {\sc i}}$/ $L_{\rm IR}$ $M_{H {\sc i}}$ / $L_{\rm B}$
  [km s-1] [Jy km s-1] [km s-1]   [10$^{\rm 9}$  $M_{\hbox{$\odot$ }}$] [10$^{\rm 10}$  $M_{\hbox{$\odot$ }}$] 10$^{\rm 10}$  $M_{\hbox{$\odot$ }}$] [ $\frac{\rm {K~km~s}^{\rm -1}{\rm pc}^{\rm 2}}{{M}_{\hbox{$\odot$ }}}$] [10$^{\rm 10}$  $L_{\hbox{$\odot$ }}$]   [ $M_{\hbox{$\odot$ }}$ pc$^{\rm -2}$] [ $M_{\hbox{$\odot$ }}$ /  $L_{\hbox{$\odot$ }}$] [ $M_{\hbox{$\odot$ }}$ /  $L_{\hbox{$\odot$ }}$]
HE 0045 6 403 3.29 $\pm$ 0.13 180.8 $\upuparrows$$_{\rm A}$ 5.7 $\pm$ 0.2 7.1 11.5 0.13 8.10 0.6 20.0 0.08 1.2
HE 0150 14 329 2.70 $\pm$ 0.28 263.0 $\upuparrows$$_{\rm A}$ 23.8 $\pm$ 2.5 45.0 26.8 0.02 11.10 0.9 27.0 0.21 4.9
HE 0212 7 921 1.97 $\pm$ 0.18 206.4 $\wedge$$_{\rm A}$ 5.3 $\pm$ 0.5 3.3 11.7 0.09 4.07 1.1 121.6 0.13 0.4
HE 0224 18 150 $2.64 \pm 0.26$ 271.0 $\sqcap$$_{\rm A}$ 37.5 $\pm$ 3.7 90.8 41.5 0.01 10.50 0.3 20.3 0.34 3.8
HE 0227 4914 $2.58 \pm 0.16$ 193.9 $\sqcap$ 2.6 $\pm$ 0.2 0.9 3.4 0.07 1.08 1.0 466.9 0.24 0.7
HE 0232 12 886 3.31 $\pm$ 0.40 559.0 $\wedge$$_{\rm A}$ $23.6 \pm 2.8$ 46.9 56.6 0.18 18.50 0.8 114.9 0.13 0.8
HE 0949 5974 5.88 $\pm$ 0.46 181.4 $\wedge$$_{\rm A}$ 8.7 $\pm$ 0.7 3.5 9.5 0.01 - 1.5 58.0 - 1.7
HE 1029 12 112 $1.05 \pm 0.10$ 241.0 $\upuparrows$ 6.6 $\pm$ 0.6 24.2 17.2 0.20 21.20 0.9 14.4 0.05 0.6
HE 1237 2531 $7.55 \pm 0.36$ 355.5 $\upuparrows$ $2.0 \pm 0.1$ 67.5 2.82 0.05 1.44 0.9 1.00 0.14 1.2
HE 1248 4338 $0.78\pm0.03$ 119.5 $\wedge$$_{\rm A}$ $1.2 \pm 0.2$d 5.7 2.2 0.08 1.29 1.4 2.6 0.12 3.5
HE 1330 6744 $1.84 \pm 0.35$ 180.4 $\upuparrows$ $3.6 \pm 0.7$ 16.1 5.0 0.05 - 1.0 6.3 - 1.6
HE 2302 14 120 $1.39 \pm 0.18$ 338.0 $\upuparrows$$_{\rm A}$ $11.9 \pm 1.5$ 130.7 19.7 0.08 - 1.3 4.7 - 1.1

Non-detections
HE 0021 15 889 <2.03 222.7   <22.2   <2.4 >0.01 -     - <4.1
HE 0040 12 390 <1.58 222.7   <10.7   <1.3 >0.03 -     - <4.2
HE 0114 13 672 <1.75 222.7   <14.0   <1.7 >0.03 -     - <2.5
HE 0119 16 291 <1.42 222.7   <16.5   <2.7 >0.08 24.6     <0.07 <1.0
HE 0253 9470 <2.58 222.7   <10.1   <1.5 >0.06 4.90     <0.21 <2.2
HE 0433 10 658 <2.21 222.7   <10.7   <2.9 >0.21 22.7     <0.05 <1.1
HE 0853 17 930 <1.03 222.7   <14.3   <2.1 >0.06 -     - <1.5
HE 1011 17 388 <0.56 222.7   <7.5   <1.5 >0.12 -     - <0.2
HE 1017 14 985 <1.22 222.7   <11.4   <1.6 >0.05 9.88     <0.12 <1.2
HE 1107 17 088 <1.03 222.7   <13.6   <1.8 >0.04 -     - <0.8
HE 1108 7199 <0.50 222.7   <1.1   <0.9 >0.85 10.4     <0.01 <0.1
HE 1126 17 988 <1.83 222.7   <25.7   <3.4 >0.04 -     - <0.5
HE 1353 10 388 <2.44 222.7   <11.4   <1.7 >0.07 -     - <4.7
HE 2222 17 431 <1.22 222.7   <15.9   <1.7 >0.01 -     - <3.7
HE 2233 16 933 <2.93 222.7   <36.1   <4.0 >0.01 -     - <4.4

a
Upper limits and errors represent 3$\sigma$ values; b for the non-detections, values of W$_{\rm 50}$ correspond to the median value of all detected sources; c line shape: $\wedge$ represents a triangular shaped line profile; A stands for asymmetries in the line profiles; spectra with $\sqcap$ show a boxy line profile; $\upuparrows$ mark line profiles of a double-horn shape; d this detection was already confirmed by follow-up observations with the VLA. The obtained value for the H I mass is $\sim$ $1.0 \times 10^{\rm 9}$  $M_{\hbox{$\odot$ }}$ (König et al. 2009).


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