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Table B.1.
Spectroscopic and information of the LTE fitting of the selected lines of o-H2NCO+ and p-H2NCO+ shown in Figure 2. The frequency, the QNs, the energy of the upper level (Eu), the logarithm of the intensity (at 300 K), , and the S/N in integrated intensity of the lines are given.
Molecule | Frequency | QNsa | Eu | log Intensity | ![]() |
S/Nb | |
---|---|---|---|---|---|---|---|
(GHz) | (K) | (nm2 MHz) | (K km s−1) | ||||
o-H2NCO+ | 40.122511 | 21, 2-11, 1 F = 1- 1 | 1.9 | -5.0506 | 0.194 | 23 | |
40.122797 | 21, 2-11, 1 F = 1- 2 | 1.9 | -6.2267 | … | … | ||
40.123224 | 21, 2-11, 1 F = 1 - 0 | 1.9 | -4.9256 | … | … | ||
40.123539 | 21, 2-11, 1 F = 3 - 2 | 1.9 | -4.3024 | … | … | ||
40.124590 | 21, 2-11, 1 F = 2 - 1 | 1.9 | -4.5734 | … | … | ||
40.124876 | 21, 2-11, 1 F = 2 - 2 | 1.9 | -5.0505 | … | … | ||
40.781503 | 21, 1-11, 0 F = 1 - 0 | 2.0 | -4.9115 | 0.116 | 17 | ||
40.782899 | 21, 1-11, 0 F = 2 - 2 | 2.0 | -5.0364 | … | … | ||
40.783205 | 21, 1-11, 0 F = 3 - 2 | 2.0 | -4.2882 | … | … | ||
40.784147 | 21, 1-11, 0 F = 2 - 1 | 2.0 | -4.5593 | … | … | ||
40.784622 | 21, 1-11, 0 F = 1 - 1 | 2.0 | -5.0364 | … | … | ||
80.246416 | 41, 4-31, 3 F = 5 - 4 | 8.7 | -3.3697 | 0.211 | 31 | ||
80.246532 | 41, 4-31, 3 F = 3 - 2 | 8.7 | -3.6030 | … | … | ||
80.246564 | 41, 4-31, 3 F = 4 - 3 | 8.7 | -3.4849 | … | … | ||
81.565492 | 41, 3-31, 2 F = 3 - 2 | 8.8 | -3.5890 | 0.209 | 31 | ||
81.565524 | 41, 3-31, 2 F = 5 - 4 | 8.8 | -3.3557 | … | … | ||
81.565633 | 41, 3-31, 2 F = 4 - 3 | 8.8 | -3.4709 | … | … | ||
101.95584 | 51, 4-41, 3 F = 4 - 3 | 13.7 | -3.0757 | 0.165 | 18 | ||
101.95585 | 51, 4-41, 3 F = 6 - 5 | 13.7 | -3.1660 | … | … | ||
101.95591 | 51, 4-41, 3 F = 5 - 4 | 13.7 | -4.5462 | … | … | ||
p-H2NCO+ | 40.453210 | 20, 2-10, 1 F = 1 - 0 | 2.9 | -4.8970 | 0.168 | 20 | |
40.454746 | 20, 2-10, 1 F = 3 - 2 | 2.9 | -4.1488 | … | … | ||
40.454815 | 20, 2-10, 1 F = 2 - 1 | 2.9 | -4.4199 | … | … | ||
40.455616 | 20, 2-10, 1 F = 1 - 0 | 2.9 | -4.7720 | … | … | ||
40.455778 | 20, 2-10, 1 F = 2 - 2 | 2.9 | -4.8970 | … | … | ||
80.906908 | 40, 4-30, 3 F = 5 - 4 | 9.7 | -3.3131 | 0.261 | |||
80.906934 | 40, 4-30, 3 F = 4 - 3 | 9.7 | -3.4283 | … | … | ||
80.907001 | 40, 4-30, 3 F = 3 - 2 | 9.7 | -3.5464 | … | … | ||
101.13112 | 50, 5-40, 4 F = 6 - 5 | 14.6 | -3.0434 | 0.213 | |||
101.13114 | 50, 5-40, 4 F = 5 - 4 | 14.6 | -3.1336 | … | … | ||
101.13117 | 50, 5-40, 4 F = 4 - 3 | 14.6 | -3.2251 | … | … | ||
101.13223 | 50, 5-40, 4 F = 5 - 5 | 14.6 | -4.5138 | … | … |
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