Table 1
Spectroscopic data and beam-averaged continuum brightness temperature assumed for the LTE modeling of the absorption lines toward Sgr B2(M).
Transition | F′−F′′a | Positionb | Frequency | S | E l | F eff c | B eff d | T cont e | Referencef | ||
(″,″) | (MHz) | (K) | (K) | ||||||||
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | ||
|
|||||||||||
c-C3H2 212–101 | 2.6,–2.0 | 85338 | .893(14) | 1.50 | 0.0g | 0.95 | 0.78 | 5.9 | JPL, h | ||
H13CO+ 1–0 | 2.6,–2.0 | 86754 | .2884(46) | 1.0 | 0.0 | 0.95 | 0.78 | 5.9 | CDMS, i | ||
CO 1–0 | 2.6,–2.0 | 115271 | .2018(5) | 1.0 | 0.0 | 0.95 | 0.74 | 5.9 | CDMS, j | ||
CO 3–2 | 2.6,–2.0 | 345795 | .9899(5) | 3.0 | 16.6 | 0.95 | 0.72 | 11.0 | CDMS, j | ||
SH+ 10–01 | 0.5−0.5 | 0,0 | 345843 | .591(128) | 0.2289 | 0.0 | 0.95 | 0.72 | 11.0 | CDMS, − | |
0.5−1.5 | 345929 | .810(75) | 0.5780 | 0.0 | CDMS, k | ||||||
H37Cl 1–0 | 1.5−1.5 | 0,0 | 624964 | .374(100) | 1.3333 | 0.0 | 0.95 | 0.41 | 33.8 | JPL, l | |
2.5−1.5 | 624977 | .821(100) | 2.0 | 0.0 | JPL, l | ||||||
0.5−1.5 | 624988 | .334(100) | 0.6667 | 0.0 | JPL, l | ||||||
H35Cl 1–0 | 1.5−1.5 | 0,0 | 625901 | .603(100) | 1.3333 | 0.0 | 0.95 | 0.41 | 33.8 | JPL, l | |
2.5−1.5 | 625918 | .756(100) | 2.0 | 0.0 | JPL, l | ||||||
0.5−1.5 | 625932 | .007(100) | 0.6667 | 0.0 | JPL, l | ||||||
SH+ 11–01 | 1.5−0.5 | 0,0 | 683336 | .08(51) | 0.1890 | 0.0 | 0.95 | 0.41 | 30.0 | CDMS, m | |
0.5−0.5 | 683361 | .98(48) | 0.3778 | 0.0 | CDMS, − | ||||||
1.5−1.5 | 683422 | .31(50) | 0.9441 | 0.0 | CDMS, m | ||||||
0.5−1.5 | 683448 | .20(50) | 0.1887 | 0.0 | CDMS, m | ||||||
13CH+ 1–0 | 0,0 | 830 216 | .096(22) | 1.0 | 0.0 | 0.95 | 0.35 | 47.7 | CDMS, n | ||
SH+ 21–11 | 0.5−0.5 | 0,0 | 893047 | .60(95) | 0.2889 | 32.8 | 0.95 | 0.35 | 43.5 | CDMS, − | |
0.5−1.5 | 893073 | .49(96) | 0.1445 | 32.8 | CDMS, − | ||||||
1.5−0.5 | 893107 | .92(105) | 0.1444 | 32.8 | CDMS, − | ||||||
1.5−1.5 | 893133 | .81(94) | 0.7225 | 32.8 | CDMS, − |
Notes.
Equatorial offset (J2000) with respect to Sgr B2(M). (0, 0) corresponds to (α,δ)J2000 = 17h47m20s.2,−28°23′05′′.
The beam-averaged continuum brightness temperature was derived from the depth of the saturated absorption lines in the 3 mm wavelength range, and from a direct measurement of the baseline level at higher frequency.
Catalog used for rest frequency and reference for line measurement, see also Sect. 2.
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