Table A.1
Parameters and results of the global fit of the spectra for non-saturated lines detected toward the SW component in 2011 ATCA observations.
Rest Freq. | Transition | S ul a | El/kBb | V 0 c | ΔVd | ∫τdVe |
(MHz) | (K) | (km s-1) | (km s-1) | (10-3 km s-1) | ||
|
||||||
87 316.898 | C2H N = 1–0 | 1.00 | 0.0 | −0.5 (0.1) | 18.9 (0.1) | 28 234 (280) |
174 663.199 | C2H N = 2–1 | 2.00 | 4.2 | –t | –t | 37 574 (486) |
86 339.922 | H13CN J = 1–0 | 1.00 | 0.0 | −2.7 (0.1) | 16.8 (0.2) | 4966 (69) |
172 677.851 | H13CN J = 2–1 | 2.00 | 4.1 | –t | –t | 6393(141) |
86 054.966 | HC15N J = 1–0 | 1.00 | 0.0 | –t | –t | 945(42) |
172 107.957 | HC15N J = 2–1 | 2.00 | 4.1 | –t | –t | 943(99) |
90 663.568 | HNC J = 1–0 | 1.00 | 0.0 | 0.17 (0.03) | 19.8 (0.1) | 43 339 (1130) |
181 324.758 | HNC J = 2–1 | 2.00 | 4.4 | –t | –t | 45 856 (1347) |
87 090.825 | HN13C J = 1–0 | 1.00 | 0.0 | –t | –t | 1515 (50) |
174 179.411 | HN13C J = 2–1 | 2.00 | 4.2 | –t | –t | 1778 (86) |
88 865.715 | H15NC J = 1–0 | 1.00 | 0.0 | –t | –t | 300 (50) |
86 754.288 | H13CO+J = 1–0 | 1.00 | 0.0 | −2.7 (0.1) | 15.6 (0.1) | 6089 (79) |
173 506.700 | H13CO+J = 2–1 | 2.00 | 4.2 | –t | –t | 8072 (153) |
85 162.223 | HC18O+J = 1–0 | 1.00 | 0.0 | –t | –t | 2581 (46) |
87 057.535 | HC17O+J = 1–0 | 1.00 | 0.0 | –t | –t | 262 (40) |
174 113.169 | HC17O+J = 2–1 | 2.00 | 4.2 | –t | –t | 231 (70) |
89 487.414 | HOC+J = 1–0 | 1.00 | 0.0 | −0.2 (0.5) | 19.3 (1.1) | 1057 (62) |
178 972.051 | HOC+J = 2–1 | 2.00 | 4.3 | –t | –t | 1283 (92) |
86 670.760 | HCO NK = 101–000J = 3/2–1/2 | 1.00 | 0.0 | −1.7 (1.0) | 18.8 (2.4) | 833 (62) |
172 266.853 | CH2NH 211–202 | 7.40 | 9.2 | −4.1 (0.6) | 9.8 (1.4) | 812 (61) |
89 956.068 | CH3NH2(p) 110–101 | 6.00 | 2.1 | −4.8 (1.5) | 12.3 (3.2) | 223 (53) |
85 338.893 | c-C3H2-o 212–101 | 4.50 | 2.3 | −1.9 (0.1) | 17.8 (0.2) | 6973 (85) |
84 727.696 | c-C3H2(p) 322–313 | 0.96 | 12.1 | –t | –t | 244 (38) |
91 958.726 | CH3CN JK = 54–44 | 3.60 | 123.1 | −3.9 (0.5) | 14.6 (1.1) | – |
91 971.130 | CH3CN JK = 53–43 | 12.80 | 73.1 | –t | –t | – |
91 979.994 | CH3CN JK = 52–42 | 8.40 | 37.4 | –t | –t | – |
91 985.314 | CH3CN JK = 51–41 | 9.60 | 16.0 | –t | –t | – |
91 987.088 | CH3CN JK = 50–40 | 10.00 | 8.8 | –t | –t | – |
87 925.237 | HNCO 404–303 | 4.00 | 6.3 | −4.5 (0.4) | 14.2 (1.0) | 845 (51) |
175 843.695 | HNCO 808–707 | 8.00 | 29.5 | –t | –t | 257 (81) |
86 846.960 | SiO J = 2–1 | 2.00 | 2.1 | −3.0 (0.1) | 14.4 (0.2) | 3612 (60) |
173 688.310 | SiO J = 4–3 | 4.00 | 12.5 | –t | –t | 1944 (96) |
85 759.199 | 29SiO J = 2–1 | 2.00 | 2.1 | –t | –t | 541 (37) |
84 746.170 | 30SiO J = 2–1 | 2.00 | 2.0 | –t | –t | 287 (35) |
85 347.890 | HCS+J = 2–1 | 2.00 | 2.0 | −1.5 (0.0)f | 15.0 (1.4) | 542 (45) |
85 531.512 | HOCO+ 404–303 | 4.00 | 6.2 | 0.5 (2.3) | 17.8 (5.5) | 181 (48) |
84 542.329 | NH2CHO 404–303 | 12.00 | 6.1 | −4.4 (0.8) | 15.0 (0.0)f | 507 (52) |
87 848.873 | NH2CHO 413–312 | 11.23 | 9.3 | –t | –t | 290 (42) |
178 605.403 | SO JK = 54–43 | 4.91 | 15.9 | −3.4 (0.7) | 13.7 (1.6) | 843 (85) |
90 979.023 | HC3N J = 10–9 | 10.00 | 19.6 | −2.5 (0.7) | 14.6 (1.6) | 680 (66) |
Notes. For some species, the fit results might be slightly different (although within uncertainties) to the values given in Table 3, due to the different fitting procedure with tied parameters.
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