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Table 2

Upper limits obtained for the Gg and Gg′ conformers of n-propanol for the anti and gauche conformers of i-propanol, and for the trans conformer of ethyl methyl ether.

Species Formula Frequency (MHz) QNs Eu (K) log I(300 K) (nm2 MHz) rms (mK) N(a) (cm−2) Abundance(b)
n-propanol (Gg) Gg-n-C3H7OH 75 699.1096 33,1 − 22,1 75.7 –6.1471 2.3 ≤1.6 × 1013(c) ≤1.2×10−10
75 700.5781 33,0−22,1 75.7 –6.2273 2.3
n-propanol (Gg′) Gg′-n-C3H7OH 87 730.9823 101,10−91,9 97.0 –5.2641 0.9 ≤5.7 × 1012 ≤4.2 × 10−11

Isopropanol (gauche) g-i-C3H7OH 88 532.3081 41,4−31,3 7.5 –5.7726 1.8 ≤8.5 × 1012 (c) ≤6.3 × 10−11
88 538.5001 40,4−30,3 7.5 –5.7737 1.8
Isopropanol (anti) a-i-C3H7OH 79 734.1627 81,8−70,7 137.9 –5.5140 2.7 ≤3.9 × 1012 (c) ≤2.9 × 10−11
79 734.1627 80,8−71,7 137.9 –5.5140 2.7

Ethyl methyl ether (trans) t-CH3OCH2CH3 73 243.2848 42,3−41,4 8.5 –5.6357 2.7 ≤3.8 × 1013 ≤2.8 × 10−10

Notes. (a)Upper limits to the column densities calculated assuming a Tex=12.5 K, i.e. the same as the one derived for Aa-n-C3H7OH, and after fixing VLSR = 69 kms−1 and Δv = 20 kms−1 (see Sect. 3.1). (b)Abundances were derived considering a H2 column density of 1.35 × 1023 cm−2 (Martín et al. 2008). (c)Upper limits were obtained considering the two transitions shown in the table, which appear blended in the spectra. The selected transitions are the cleanest and the brightest of all the lines covered in our observations.

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