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Diffuse interstellar clouds present an active chemistry despite their relatively low density and the ubiquitous presence of far-UV radiation. To provide constraints on the chemical processes responsible for the observed columns of organic species, we used the NOEMA interferometer to observe the sight line toward NRAO150 (B0355+508) in the 2mm spectral window. We targeted the low excitation lines of ortho H$_2$CO ($2_ $) and para H$_2$CO ($2_ $) as well as the nearby transitions of CS($3-2$) and c-C$_3$H$_2$ ($3_ $), and ($2_ $). We combined these data with previous observations of the same sight line to determine the excitation conditions, column densities, and abundances relative to H$_2$ in the different velocity components. We performed non-LTE radiative transfer calculations including collision cross sections with ortho and para H$_2$ and with electrons. New collision cross sections with electrons were computed for ortho and para formaldehyde. All targeted lines were detected. The c-C$_3$H$_2$ line profiles are very similar to those of HCO$^+$ and CCH, while the CS absorption features are narrower and mostly concentrated in two main velocity components at V$_ LSR $ = -17.2 and -10.4 H$_2$CO absorption lines present an intermediate pattern with absorption in all velocity components but larger opacities in the two main velocity components. The ortho-to-para ratios of H$_2$CO and c-C$_3$H$_2$ are consistent with the statistical value of three. While the excitation temperature of all c-C$_3$H$_2$ velocity components is consistent with the Cosmic Microwave Background (CMB), the two strong components detected in CS show a clear excess over the CMB indicating that CS resides at higher densities than other species along this particular sightline, n(H$_2$) $ $ while n(H$_2$) $< 500$ cm$^ $ for the other velocity components. We detected faint absorption from o-H$_2$13CO and C34S allowing us to derive isotopic ratios: o-H$_2$CO/o-H$_2$13CO = $61 12$ and C32S/C34S = $24 The excitation of the $ line of formaldehyde at 4.8 GHz is sensitive to the electron fraction and its excitation temperature is predicted to be lower than the CMB at low and moderate electron fractions ($x(e) < 6 $), and to rise above the CMB at high electron fractions ($x(e) > 10^
Diffuse interstellar clouds present an active chemistry despite their relatively low density and the ubiquitous presence of far-UV radiation. To provide constraints on the chemical processes responsible for the observed columns of organic species, we used the NOEMA interferometer to observe the sight line toward NRAO150 (B0355+508) in the 2mm spectral window. We targeted the low excitation lines of ortho H$_2$CO ($2_ $) and para H$_2$CO ($2_ $) as well as the nearby transitions of CS($3-2$) and c-C$_3$H$_2$ ($3_ $), and ($2_ $). We combined these data with previous observations of the same sight line to determine the excitation conditions, column densities, and abundances relative to H$_2$ in the different velocity components. We performed non-LTE radiative transfer calculations including collision cross sections with ortho and para H$_2$ and with electrons. New collision cross sections with electrons were computed for ortho and para formaldehyde. All targeted lines were detected. The c-C$_3$H$_2$ line profiles are very similar to those of HCO$^+$ and CCH, while the CS absorption features are narrower and mostly concentrated in two main velocity components at V$_ LSR $ = -17.2 and -10.4 H$_2$CO absorption lines present an intermediate pattern with absorption in all velocity components but larger opacities in the two main velocity components. The ortho-to-para ratios of H$_2$CO and c-C$_3$H$_2$ are consistent with the statistical value of three. While the excitation temperature of all c-C$_3$H$_2$ velocity components is consistent with the Cosmic Microwave Background (CMB), the two strong components detected in CS show a clear excess over the CMB indicating that CS resides at higher densities than other species along this particular sightline, n(H$_2$) $ $ while n(H$_2$) $< 500$ cm$^ $ for the other velocity components. We detected faint absorption from o-H$_2$13CO and C34S allowing us to derive isotopic ratios: o-H$_2$CO/o-H$_2$13CO = $61 12$ and C32S/C34S = $24 The excitation of the $ line of formaldehyde at 4.8 GHz is sensitive to the electron fraction and its excitation temperature is predicted to be lower than the CMB at low and moderate electron fractions ($x(e) < 6 $), and to rise above the CMB at high electron fractions ($x(e) > 10^
The systematic analysis of the correlations between diffuse interstellar bands (DIBs) is extended to weak DIBs through the comprehensive catalogue of the Apache Peak Observatory (APO) of 559 DIBs in 25 lines of sight with diverse interstellar properties. The main results are the following: 1) An extension of the number of DIBs identified to be related to C2, that is, those that need very shielded interstellar regions for their carriers to survive UV photo-dissociation. Based on the correlations with the reference C2 and ζ DIBs, anticorrelations with UV-favoured (σ) DIBs, and the strength ratios in shielded and unshielded sight lines, we propose 12 new C2 candidates and 34 possible “C2-related” DIBs (mostly at λ <5950 Å) in addition to the ~20 known confirmed C2 DIBs. With these additions, the census of C2 DIBs might approach completion. 2) We discovered that the intensities of a large set of poorly studied DIBs are strongly enhanced in one or two of the sight lines of HD 175156 and HD 148579. This tentative class, denoted χ for the time being, extends over the whole wavelength range of visible DIBs. It might include up to 50–100 members, half at λ > 6000 Å, and a number of C2 DIBs. These possible enhancements might reflect specific formation processes of their carriers that are yet to be identified in the interstellar medium of these two sight lines. The possible matches of the wavelength of five very broad DIBs, including three χ DIBs, with the strong bands that were recently measured by action spectroscopy might favour some long carbon chains and rings as carriers of some DIBs. These correlations and findings justify further theoretical and laboratory efforts for improving our understanding of the complex physics, spectroscopy, and chemistry of the various carbon chains and rings, and their possible formation and destruction in the diffuse interstellar medium.
Improved opacities are needed for modelling the atmospheres and evolution of cool carbon-rich stars and extra-solar planets; in particular, contributions made by the astrophysically important propadienediylidene (C3) molecule need, at a minimum, to be determined using a line list which includes all significant transitions in the energy range of interest. We report variational calculations giving ro-vibrational energy levels and corresponding line-strengths for 12C3, 12C13C12C and 12C12C13C. In the 12C3 case we obtain 2 166 503 ro-vibrational state energies ≤20000 cm−1 for the electronic $\tilde{X}{\, }^{1}{\Sigma _{\rm g}}^{+}$ ground-state. Comparison with experiment indicates a maximum error of ±0.03 cm−1 in calculated positions of lines involving an upper state energy ⪅4000 cm−1. For lines with upper state energies ⪆4000 cm−1 to have comparable line-position accuracies, conical intersections would need to be accounted for in an adopted potential energy surface. Line lists and associated opacities are provided in the ExoMol Database (http://www.exomol.com).
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