2017
DOI: 10.1093/mnras/stx1331
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Collisional excitation of NH3 by atomic and molecular hydrogen

Abstract: We report extensive theoretical calculations on the rotation-inversion excitation of interstellar ammonia (NH 3 ) due to collisions with atomic and molecular hydrogen (both para-and ortho-H 2 ). Close-coupling calculations are performed for total energies in the range 1-2000 cm −1 and rotational cross sections are obtained for all transitions among the lowest 17 and 34 rotation-inversion levels of ortho-and para-NH 3 , respectively. Rate coefficients are deduced for kinetic temperatures up to 200 K. Propensity… Show more

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Cited by 32 publications
(62 citation statements)
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“…We took into account the hyperfine structure, produced by the electric quadrupole coupling of the N nucleus with the electric field of the electrons, as well as the magnetic hyperfine structure that is due to the three protons (Cazzoli et al 2009). The hyperfine collision rate coefficients were taken from the recent calculations of Bouhafs et al (2017), which, for the first time, include the non-spherical structure of p-H 2 (the main form of H 2 in cold molecular gas, Flower et al 2006;Brünken et al 2014), so that they differ (by up to a factor 2) from those of Maret et al (2009). The calculations were restricted to the lowest nine hyperfine levels of o-NH 3 , corresponding to the first two rotational levels (0 0 and 1 0 ), within a temperature range 5−30 K. Since only the ground-state o-NH 3 transitions were considered, no scaling of the rotational rates was necessary: all hyperfine rates are equal to the pure rotational rates, and intra-multiplet rates are set to zero, as in the standard statistical approach.…”
Section: Discussionmentioning
confidence: 99%
“…We took into account the hyperfine structure, produced by the electric quadrupole coupling of the N nucleus with the electric field of the electrons, as well as the magnetic hyperfine structure that is due to the three protons (Cazzoli et al 2009). The hyperfine collision rate coefficients were taken from the recent calculations of Bouhafs et al (2017), which, for the first time, include the non-spherical structure of p-H 2 (the main form of H 2 in cold molecular gas, Flower et al 2006;Brünken et al 2014), so that they differ (by up to a factor 2) from those of Maret et al (2009). The calculations were restricted to the lowest nine hyperfine levels of o-NH 3 , corresponding to the first two rotational levels (0 0 and 1 0 ), within a temperature range 5−30 K. Since only the ground-state o-NH 3 transitions were considered, no scaling of the rotational rates was necessary: all hyperfine rates are equal to the pure rotational rates, and intra-multiplet rates are set to zero, as in the standard statistical approach.…”
Section: Discussionmentioning
confidence: 99%
“…Similar to the analysis of Schmidt et al (2016, their Sect. 3), we compare the synthesised spectra of the transitions discussed in this article using the above-mentioned extended coefficients with those using only the coefficients of either Danby et al (1988) or Bouhafs et al (2017). Neglecting collisional transitions of high-J and 2 -excited levels, the coefficients of Danby et al (1988) and Bouhafs et al (2017) do not produce qualitatively different spectra. While the spectra of IK Tau are insensitive to the presence of the extended rate coefficients, those of the other targets are noticeably affected, especially in the rotational transitions (<50% in the peak intensity).…”
Section: Notesmentioning
confidence: 99%
“…By adopting some constant rate coefficients for other transitions, Schmidt et al (2016) found that the collisional transitions involving higher ground-state levels or vibrationally excited levels were not important. Bouhafs et al (2017) reported new calculations on the rate coefficients of the collisions between NH 3 and atomic hydrogen (H), ortho-H 2 , and para-H 2 at temperatures up to 200 K and in transitions involving energy levels up to E up /k = 600 K (J ortho ≤ 6 and J para ≤ 7). Their calculations were based on the full-dimensional (9-D) NH 3 -H potential energy surface (PES) of Li & Guo (2014) and the five-dimensional NH 3 -H 2 PES of Maret et al (2009) with an ad hoc approximation of the inversion wave functions using the method of Green (1976).…”
Section: Collisional Rate Coefficientsmentioning
confidence: 99%
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