Table 2
Line parameters and derived optical depths.
Transition | ν observed | ν rest | V | ΔV | f c | τ | τ | Δτ | Remarks |
(GHz) | (km s-1) | fc = .38 | |||||||
|
|||||||||
Our detections | |||||||||
H2CO 312 ← 313(o) | 15.36456 | 28.97480 | 8.9 ± 2.7 | 27.1 ± 5.3 | .153 | .054 | .021 | 30% | 070 801 |
SO 10 ← 01 | 15.90902 | 30.00154 | 7.5 ± 0.4 | 5.4 ± 1.2 | .156 | .031 | .013 | 10% | 140 801, 1 |
5.8 ± 2.4 | 37.2 ± 5.8 | .156 | .016 | .006 | 25% | 140 801, 1 | |||
c−C3H2 110 ← 101(o) | 18.34314 | 18.34314 | 4.6 ± 0.6 | 5.1 ± 1.5 | 1.00 | .007 | – | ≳ 30% | 151 201, 2 |
CH3OH 10 ← 00(A+) | 25.65063 | 48.37247 | 8.7 ± 0.5 | 8.3 ± 1.4 | .196 | .065 | .033 | 20% | 231 201, 3 |
CH3OH 10 ← 00(E) | 25.65297 | 48.37689 | 8.7 ± 1.3 | 5.1 ± 4.9 | .196 | .020 | .010 | 100% | 231 201, 3 |
c−C3H2 111 ← 000(p) | 27.49012 | 51.84141 | 10.2 ± 0.7 | 15.4 ± 2.3 | .198 | .097 | .050 | 20% | 290 901 |
SO 21 ← 10 | 33.37105 | 62.93179 | 8.6 ± 1.1 | 20.9 ± 2.5 | .227 | .063 | .038 | 20% | 011 001 |
|
|||||||||
Our nondetections | |||||||||
HC5N 13 ← 12 | 18.35508 | 34.61439 | – | – | .17 | <.003 | <.001 | 7% | 151 201, 4 |
SiS 2 ← 1 | 19.25403 | 36.30963 | – | – | .17 | <.002 | <.001 | 7% | 151 201, 4 |
H56α | 19.33709 | 36.46627 | – | – | .17 | <.018 | <.008 | 7% | 151 201, 4 |
H70β | 19.49376 | 36.76172 | – | – | .17 | <.018 | <.008 | 7% | 151 201, 4 |
HNCO 202 ← 101 | 23.31249 | 43.96300 | – | – | .19 | <.004 | <.002 | 7% | 301 201, 4 |
HC5N 20 ← 19 | 28.23830 | 53.25235 | – | – | .21 | <.005 | <.003 | 7% | 031 001, 4 |
SO2 211 ← 202 | 28.38493 | 53.52887 | – | – | .22 | <.006 | <.004 | 7% | 031 001, 4 |
SO 34 ← 33 | 35.01657 | 66.03494 | – | – | .23 | <.009 | <.006 | 7% | 021 001, 4 |
|
|||||||||
Menten et al. (1999) | |||||||||
H2CO 211 ← 212(o) | 07.68285 | 14.48848 | ~9 | ~20 | .20 | .050 | .026 | 15% | 5 |
c−C3H2 212 ← 101 (o) | 45.25294 | 85.33891 | ~9 | ~20 | .35 | .210 | .190 | 15% | 5, 7 |
|
|||||||||
Muller et al. (2011) | |||||||||
c−C3H2 331 ← 322(p) | 31.58196 | 59.55789 | – | – | .22 | .005 | .003 | 20% | 6 |
CH3OH 10 ← 2-1 (E) | 32.09821 | 60.53146 | 7.1 ± 0.5 | 21.2 ± 1.2 | .22 | .033 | .019 | 10% | 6 |
SO 21 ← 10 | 33.37105 | 62.93180 | 11.4 ± 0.3 | 19.7 ± 0.7 | .23 | .050 | .030 | 10% | 6 |
c−C3H2 202 ← 111(p) | 43.53202 | 82.09356 | – | – | .26 | .084 | .057 | 10% | 6 |
c−C3H2 312 ← 303(o) | 43.99476 | 82.96621 | 11.5 ± 0.1 | 18.7 ± 0.2 | .26 | .031 | .022 | 10% | 6 |
c−C3H2 212 ← 101(o) | 45.25294 | 85.33891 | – | – | .26 | .285 | .189 | 10% | 6, 7 |
SO 22 ← 11 | 45.65332 | 86.09395 | – | – | .27 | .004 | .003 | 35% | 6 |
Notes. “Our detections” and “Our nondetections” were all obtained between August and December 2001. Col. (1): molecular line, (o) = ortho, (p) = para; Col. (2): redshifted frequency, adopting z = 0.88582; Col. (3): approximate rest frequency; Cols. (4) and (5): local standard of rest velocities and full width to half power (FWHP) line widths, in case of SO 10 ← 01 for both the broad and the narrow component; Cols. (6) and (7): continuum source-covering factor (see also Sect. 4.1 and Henkel et al. 2009) and corresponding peak optical depth(s); Col. (8): peak optical depths for a continuum source-covering factor of 0.38; Col. (9): estimated 1σ uncertainties in percent of the optical depth. Remarks (last column): the 6-digit numbers provide the epoch of our observations with day, month, and year from left to right. 1: possibly two line components. 2: Galactic line, tentative detection. A continuum source-covering factor of unity has been adopted. 3: E- and A-transitions seen in the same spectrum (Fig. 1). The intensities are consistent with a line strength ratio of 1:3.8. 4: upper 1σ limits of τ; spectra were smoothed to ~10 km s-1 channels. 5: extrapolated continuum flux densities: 7.1 Jy (14 GHz) and 3.5 Jy (45 GHz). 6: calculated from Table 10 of Muller et al. (2011). 7: τ values of Menten et al. (1999) and Muller et al. (2011) agree well.
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