Table 8
Derived column densities over specific velocity intervals.
Source | υLSR range (km s−1) | N(H2) (1021 cm−2) | N(HCO+) (1012 cm−2) | N(HCN) (1012 cm−2) | N(HNC) (1012 cm−2) | N(CS) (1012 cm−2) | N(H2S) (1013 cm−2) | N(C2H) (1013 cm−2) | N(c-C3H2) (1012 cm−2) |
---|---|---|---|---|---|---|---|---|---|
W3 IRS5 | −24, −18 | ![]() |
![]() |
![]() |
… | … | … | ![]() |
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−6, −1 | ![]() |
![]() |
… | … | … | … | … | … | |
−1, 5 | ![]() |
![]() |
… | … | … | … | … | … | |
W3(OH) | −23, −15 | ![]() |
![]() |
![]() |
… | … | … | ![]() |
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−14, −7 | ![]() |
![]() |
![]() |
![]() |
… | … | ![]() |
![]() |
|
−7, 3 | ![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
![]() |
|
NGC 6334 I | 0, 12(a) | ![]() |
![]() |
![]() |
![]() |
… | … | ![]() |
![]() |
HGAL0.55−0.85 | −14, −4(a) | ![]() |
![]() |
… | … | … | … | … | … |
G09.62+0.19 | 9, 20 | ![]() |
![]() |
![]() |
![]() |
… | ![]() |
… | … |
20, 29 | ![]() |
![]() |
![]() |
![]() |
… | ![]() |
![]() |
… | |
62, 73 | ![]() |
![]() |
… | … | … | … | … | … | |
G10.47+0.03 | −18, −9 | ![]() |
![]() |
![]() |
… | … | … | … | … |
−9, 3 | ![]() |
![]() |
![]() |
… | ![]() |
… | … | … | |
3, 7 | ![]() |
![]() |
![]() |
![]() |
![]() |
… | ![]() |
… | |
7, 14 | ![]() |
![]() |
![]() |
![]() |
![]() |
… | ![]() |
… | |
14, 19 | ![]() |
![]() |
![]() |
![]() |
… | … | ![]() |
… | |
19, 28 | ![]() |
![]() |
![]() |
… | … | … | ![]() |
… | |
28, 32 | ![]() |
![]() |
![]() |
… | … | … | ![]() |
… | |
32, 44 | ![]() |
![]() |
![]() |
![]() |
… | … | ![]() |
… | |
44, 51 | ![]() |
![]() |
… | … | … | … | … | … | |
82, 94 | ![]() |
![]() |
![]() |
… | … | … | … | … | |
114, 133 | ![]() |
![]() |
![]() |
… | ![]() |
… | … | … | |
137, 151 | ![]() |
![]() |
![]() |
… | ![]() |
… | … | … | |
151, 159 | ![]() |
![]() |
![]() |
![]() |
![]() |
… | ![]() |
… | |
159, 164 | ![]() |
![]() |
![]() |
… | ![]() |
… | … | … | |
164, 175 | ![]() |
![]() |
![]() |
… | ![]() |
… | … | … |
Notes. N(H2) is derived using N(HCO+); N(H2) = N(HCO+)/ 3 × 10−9 for a case with N(HCO+) < 2.8 × 1012 cm−2, N(H2) = N(HCO+)/2 × 10−8 for a case with N(HCO+) > 9.4 × 1013 cm−2, and an interpolated value between these two ranges of N(HCO+), log(N(H2)) = log(N(HCO+))×1.64. The column densities derived for each species toward the remaining sources is tabulated in Appendix B. The velocity intervals are defined, based on HCO+ absorption line profiles. (a)Refers to the velocity intervals corresponding to molecular gas components associated with the background continuum sources, and thus the derived column densities of these velocity intervals indicate lower limits. (b)Indicates the N(H2) for the velocity intervals belonging to the GC region where likely have higher X(HCO+) (>3.9 × 10−9 for the central molecular zone Riquelme et al. 2018) than the Galactic disk regions.
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