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Table 6

Spectroscopic properties of CH3CONH2 lines detected in PRIMOS toward Sgr B2(LMH).

Transitions Symm. Frequency Eup Sijμ2 Transition
F′−F (MHz) (K) (D2) type
1(1,0) – 1(0,1) F = 1–1 A 6357.895(8) 0.9988 1.595 bQ1,−1
F = 1–2 A 6358.472(7) 0.9988 2.658
F = 2–1 A 6359.078(6) 0.9989 2.657
F = 1–0 A 6359.338(8) 0.9988 2.126
F = 2–2 A 6359.656(5) 0.9989 7.973
F = 0–1 A 6360.853(8) 0.9990 2.125
2(1,1) - 1(1,0) E 9050.672(1) 8.8659 4.154 aP0,1
2(2,0) – 2(1,1) F = 2–1 A 9252.990(7) 3.0293 1.247 bQ1,−1
F = 2–3 A 9253.351(6) 3.0293 1.294
F = 2–2 A 9254.000(6) 3.0293 5.771
F = 3–3 A 9254.535(4) 3.0293 10.339
F = 1–1 A 9254.833(6) 3.0294 3.738
F = 3–2 A 9255.185(6) 3.0293 1.293
F = 1–2 A 9255.843(7) 3.0294 1.246
1(1,1) - 1(0,1) E 13 388.703(1) 7.4374 7.644 aQ1,0
4(3,1) – 4(2,2) F = 4–3 A 14 209.211(10) 9.3165 0.749 bQ1,−1
F = 4–5 A 14 209.393(9) 9.3165 0.753
F = 4–4 A 14 210.101(7) 9.3165 13.901
F = 5–5 A 14 210.440(7) 9.3165 18.072
F = 3–3 A 14 210.527(7) 9.3165 11.233
F = 5–4 A 14 211.147(9) 9.3165 0.753
F = 3–4 A 14 211.416(10) 9.3165 0.749
3(3,0) – 3(2,1) A 14 441.706(1) 6.1401 24.436 bQ1,−1
2(1,2) – 1(1,1) E 14 651.890(1) 8.1405 11.226 aP0,1
3(1,2) – 3(1,3) E 14 960.874(1) 10.4612 4.369 aQ0,−1
2(1,1) – 2(1,2) E 15 115.748(1) 8.8659 13.673 aQ0,−1
4(3,2) – 4(2,2) E 18 507.373(2) 15.0377 23.916 bQ1,0
6(4,2) – 6(3,3) A 19 422.841(1) 19.0778 65.746 bQ1,−1
5(3,2) – 5(2,3) A 19 463.627(1) 13.3666 49.517 bQ1,−1
3(2,1) – 3(2,2) E 20 686.104(1) 12.0580 23.052 aQ0,−1
2(2,1) – 2(1,1) E 20 891.602(1) 9.8686 16.739 bQ1,0
4(2,2) – 4(1,3) A 21 362.137(1) 8.6346 30.887 bQ1,−1
4(4,0) – 4(3,1) A 21 762.725(2) 10.3609 22.240 bQ1,−1
2(0,2) – 1(0,1) E 22 095.527(1) 7.8551 18.829 aP0,1
3(3,1) – 3(2,2) A 22 769.640(1) 6.0783 16.040 bQ1,−1
6(5,1) – 6(4,2) A 25 149.383(2) 20.2848 45.460 bQ1,−1
4(3,1) – 4(3,2) E 26 196.049(1) 16.2949 30.516 aQ0,−1

Notes. CH3CONH2 rest frequencies from Ilyushin (2004) and F. J. Lovas, priv. comm. Uncertainties in parentheses refer to the least significant digit and are 2σ values (type A coverage) (Taylor & Kuyatt 1994).

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