Table 2
Observed properties of the [O I] jet from FIR 3.
Position | RA(J2000) | Dec(J2000) | [O I] 63 μma | Mass-loss rate | [O I] 63 μm/145 μm | Electron density | |
along the jet | Line flux | Line luminosity | Ṁ out | flux ratiob | n e | ||
(× 10-15 Wm-2) | (× 10-2L⊙) | (× 10-6M⊙ yr-1) | (× 104cm-3) | ||||
|
|||||||
FIR 4 | 5 35 27.07 | −5 10 0.37 | 5.1 ± 0.14 | 2.8 | 2.3 | 12.2 ± 0.7 | 4.8 ± 0.7 |
JetSW | 5 35 27.48 | −5 09 44.64 | 5.2 ± 0.14 | 2.8 | 2.3 | 13.5 ± 0.8 | 6.5 ± 0.9 |
FIR 3 | 5 35 27.67 | −5 09 35.10 | 4.8 ± 0.14 | 2.6 | 2.1 | 14.1 ± 1.0 | 7.4 ± 1.1 |
JetNE | 5 35 27.74 | −5 09 20.70 | 3.8 ± 0.14 | 2.1 | 1.7 | 13.8 ± 1.2 | 7.0 ± 1.4 |
cEntire jet | 17.3 ± 0.3 | 9.5 | 7.7 |
Notes.
The [O I] 63 line fluxes are extracted using a 9′′ radius aperture at the indicated positions. The statistical uncertainties in the line flux are estimated from the rms noise in the background-subtracted line maps. The line luminosities and mass-loss rates have the same fractional uncertainty as the line flux fractional uncertainty. The systematic uncertainties in the line flux for unchopped observations are dominated by the calibration errors and are expected to be ≲10–12%.
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