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Table 4

H2 and [Fe ii] jet widths and opening angles.

1 2 3 4 5 6 7 8 9 10 11 12
Source Lbola Offset WH2b θH2c Ranged θH2(fit)d Offset W [FeII] b θ [FeII] c Ranged θ [FeII] (fit)d
(L) (AU) (arcsec) (deg) (AU) (deg) (AU) (arcsec) (deg) (AU) (deg)

HH 34-IRS 12–45 48.5 0.17  < 48 0-640 42( ± 4) 48.5 0.19  < 84 ... ...
HH 300-IRS 1.1–1.3 ... ... ... ... ... ... ... ... ... ...
SVS13 50–80 103 0.35  < 41 0-350 21( ± 4) 68.5 0.17  < 30 0-280 22( ± 2)
HH 72-IRS 170–280 212 0.27  < 87 ... ... 212 0.22  < 76 0-1700 25( ± 3)
HH 999-IRS 6.0 141 0.24  < 46 0-780 37( ± 6) 282 0.30  < 30 0-850 27( ± 3)
HH 26-IRS 4.6–9.2 44.1 0.14  < 65 0-530 28( ± 2) ... ... ... ... ...
HH 83-IRS 10.5 ... ... ... ... ... .. ... ... ... ...

Notes. 

(a)

Source bolometric luminosity taken from the literature: see Reipurth (1989), Chrysostomou et al. (2000), Yun et al. (2001) and Antoniucci et al. (2008).

(b)

FWHM widths of the H2 and [Fe ii] flow components measured at the distances listed in Cols. 3 and 8, respectively. Values are corrected for seeing (see Fig. 4).

(c)

Upper limits on the flow component (full) opening angles, θH2 and θ [FeII] , derived from the offsets and widths in Cols. 3, 4 (for H2) and 8, 9 (for [Fe ii]).

(d)

Flow component full opening angles derived from fits to the jet widths plotted in Fig. 4 (which have been corrected for seeing) over the range specified in Cols. 6 and 11.

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