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Table 2:

Submillimetre sources in the Ori B9 cloud.
  Peak position $S_{870}^{\rm peak}$ S870 $\theta_{\rm s}$  
Name $\alpha_{2000.0}$ [h:m:s] $\delta_{2000.0}$ [ $\hbox{$^\circ$ }$: $\hbox{$^\prime$ }$: $\hbox{$^{\prime\prime}$ }$] [Jy beam-1] [Jy] [ $^{\prime\prime}$] Axis ratio
IRAS 05399-0121 05 42 27.4 -01 19 50 0.81 $2.7\pm0.3$ $30\pm4$ 1.3
SMM 1 05 42 30.5 -01 20 45 0.41 $3.0\pm0.3$ $57\pm7$ 2.5
SMM 2 05 42 32.9 -01 25 28 0.21 $0.7\pm0.1$ $26\pm5$ 3.8
SMM 3 05 42 44.4 -01 16 03 1.14 $2.5\pm0.4$ $19\pm3$ 1.5
IRAS 05405-0117 05 43 02.7 -01 16 21 0.19 $0.9\pm0.1$a $45\pm8$ a 1.2
SMM 4 05 43 03.9 -01 15 44 0.28 $1.3\pm0.1$ $34\pm6$ 2.3
SMM 5 05 43 04.5 -01 17 06 0.16 $0.6\pm0.1$ $38\pm4$ 1.8
SMM 6 05 43 05.1 -01 18 38 0.26 $2.5\pm0.3$ $92\pm35$ 4.1
Ori B9 N 05 43 05.7 -01 14 41 0.16 $1.0\pm0.1$ $47\pm5$ 1.2
SMM 7 05 43 22.1 -01 13 46 0.32 $0.8\pm0.1$ $24\pm4$ 1.8
IRAS 05412-0105 05 43 46.4 -01 04 30 0.17 $0.5\pm0.1$ - -
IRAS 05413-0104 05 43 51.3 -01 02 50 0.66 $0.9\pm0.2$ $25\pm8$ 1.6

a These values include both the IRAS 05405-0117 and Ori B9 E (see text and Fig. 3).


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