Chemical Complexity of Phosphorous-bearing Species in Various Regions of the Interstellar Medium

M Sil, S Srivastav, B Bhat, SK Mondal… - The Astronomical …, 2021 - iopscience.iop.org
The Astronomical Journal, 2021iopscience.iop.org
Phosphorus-related species are not known to be as omnipresent in space as hydrogen,
carbon, nitrogen, oxygen, and sulfur-bearing species. Astronomers spotted very few P-
bearing molecules in the interstellar medium and circumstellar envelopes. Limited discovery
of the P-bearing species imposes severe constraints in modeling the P-chemistry. In this
paper, we carry out extensive chemical models to follow the fate of P-bearing species in
diffuse clouds, photon-dominated or photodissociation regions (PDRs), and hot …
Abstract
Phosphorus-related species are not known to be as omnipresent in space as hydrogen, carbon, nitrogen, oxygen, and sulfur-bearing species. Astronomers spotted very few P-bearing molecules in the interstellar medium and circumstellar envelopes. Limited discovery of the P-bearing species imposes severe constraints in modeling the P-chemistry. In this paper, we carry out extensive chemical models to follow the fate of P-bearing species in diffuse clouds, photon-dominated or photodissociation regions (PDRs), and hot cores/corinos. We notice a curious correlation between the abundances of PO and PN and atomic nitrogen. Since N atoms are more abundant in diffuse clouds and PDRs than in the hot core/corino region, PO/PN reflects< 1 in diffuse clouds,≪ 1 in PDRs, and> 1 in the late warm-up evolutionary stage of the hot core/corino regions. During the end of the post-warm-up stage, we obtain PO/PN> 1 for hot core and< 1 for its low-mass analog. We employ a radiative transfer model to investigate the transitions of some of the P-bearing species in diffuse cloud and hot core regions and estimate the line profiles. Our study estimates the required integration time to observe these transitions with ground-based and space-based telescopes. We also carry out quantum chemical computation of the infrared features of PH 3, along with various impurities. We notice that SO 2 overlaps with the PH 3 bending-scissoring modes around∼ 1000–1100 cm− 1. We also find that the presence of CO 2 can strongly influence the intensity of the stretching modes around∼ 2400 cm− 1 of PH 3.
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