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Table 3

Selected lines of the two forms of vinyl alcohol (H2C=CHOH), syn (s) and anti (a) detected towards G+0.693.

Frequency (MHz) QNs Eu (K) log 1(300K) (nm2MHz) rms (mK) δv (kms−1) (Kkms−1) S/N Blending
s-H2C=CHOH

37 459.19(*) 21 ,2−11,1 5.09 –6.3478 1.1 2.0 0.103(0.007)(c) 14.7 Clean transition(b)
39 016.31(*) 20,2−10,1 2.81 –6.1842 1.2 1.9 0.193(0.007) 25.9 Clean transition(b)
40 650.65(*) 21 ,1−11,0 5.32 –6.2770 1.3 1.9 0.109(0.008) 13.8 Clean transition(b)
74 842.40(*) 41,4−31,3 11.38 –5.3566 3.2 2.4 0.244(0.022) 10.9 Slightly blended with t-HCOOH and HCCHO(b)
86 557.56(*) 21 ,2−10,1 5.09 –5.3840 2.4 2.1 0.454(0.016) 29.1 Slightly blended with t-HCOOH and c-HCOOH(b)
142 348.06(*) 42,2−41,3 18.98 –4.7860 3.4 1.7 0.199(0.020) 10.0 Blended with C2H5CN
151 085.05(*) 61,6−50,5 21.24 –4.5207 4.1 1.6 0.261(0.023) 11.2 Slightly blended with C2H5CHO(b)
154 490.28(*) 32,2−31,3 15.20 –4.9105 4.3 1.6 0.227(0.024) 9.4 Blended with C2H3CN
161 794.81 52,4−51,5 23.63 –4.6522 3.1 6.0 0.13(0.04) 3.1 Clean transition

a-H2C=CHOH

72 576.63 60,6−51,5 19.5 –4.6023 2.0 5.0 0.096(0.021) 4.7 Clean transition
77 015.59(*) 71 ,6−70,7 29.6 –4.2548 2.2 2.4 0.101(0.015) 6.6 Slightly blended with a-13CH3CH2OH(b)
89 757.10(*) 21 ,2−10,1 5.2 –4.6954 2.1 2.0 0.167(0.013) 12.6 Clean transition(b)
94 064.95 91,8−90,9 46.0 –4.0615 1.7 1.9 0.043(0.011) 4.0 Clean transition
106 949.48(*) 31,3−20,2 7.9 –4.4184 2.7 1.7 0.224(0.016) 14.5 Clean transition(b)
139 916.89(*) 90,9−81,8 41.5 –3.8023 2.1 1.7 0.074(0.012) 6.1 Clean transition
152 530.51 42,2−41,3 19.6 –4.0754 1.9 6.4 0.162(0.022) 7.5(d) Clean transition(b)
155 160.66 32,1−31,2 15.8 –4.2142 2.1 6.4 0.149(0.024) 6.3(d) Blended with CH3CHO(b)
232 655.55 42,3−31,2 19.5 –3.7853 4.5 8.3 0.21(0.06) 3.7 Clean transition

Notes. (a)The S/N are calculated from the integrated intensity of the lines inferred from the LTE fits of MADCUBA-SLIM. They are not calculated from the Gaussian fits of individual lines. (b)These transitions have been detected at the ≥3rms noise level in peak intensity. (c)The error in the integrated intensity is calculated as , with δv the velocity resolution of the spectra and Δv the FWHM of the line emission of 20 km s−1. (d)This S/N should be taken with caution since the LTE fit carried out by MADCUBA-SLIM overpredicts the integrated intensity of the line.(*)Transitions that provide the identification of the species with S/N ≥ 6 in integrated intensity.

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