Abstract

We carried out a sensitive survey of C2_2 and C3_3 using the EDIBLES data set. We also expanded our searches to C4_4, C5_5, and 13^{13}C12^{12}C isotopologue in the most molecule-rich sightlines. We fit synthetic spectra generated following a physical excitation model to the C2_2 (2-0) Phillips band to obtain the C2_2 column density (NN) as well as the kinetic temperature (TkinT_\textrm{kin}) and number density (nn) of the host cloud. The C3_3 molecule was measured through its A~X~\tilde{A} - \tilde{X} (000-000) electronic origin band system. We simulated the excitation of this band with a double-temperature Boltzmann distribution. We present the largest combined survey of C2_2 and C3_3 to date in which the individual transitions can be resolved. In total we detected C2_2 in 51 velocity components along 40 sightlines, and C3_3 in 31 velocity components along 27 sightlines. The two molecules are detected in the same velocity components. We find a very good correlation between NN(C2_2) and NN(C3_3) with Pearson r=0.93r = 0.93 and an average NN(C2_2)/NN(C3_3) ratio of 15.5±\pm1.4. A comparison with the behaviour of the C2_2 DIBs shows that there are no clear differences among sightlines with and without detection of C2_2 and C3_3. This is in direct contrast to the better-studied non-C2_2 DIBs who have reduced strengths in molecule-rich environments. We also identify for the first time the QQ(2), QQ(3), and QQ(4) transitions of the 13^{13}C12^{12}C (2-0) Phillips band in a stacked average spectrum, and estimate the isotopic ratio of carbon 12^{12}C/13^{13}C as 79±\pm8. Our search for the C4_4 and C5_5 optical bands was unsuccessful.Comment: 31 pages, 23 figures. To appear in A&

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