HCN/HNC chemistry in shocks: a study of L1157-B1 with ASAI

Author:

Lefloch B1ORCID,Busquet G123,Viti S45,Vastel C6,Mendoza E7,Benedettini M8,Codella C19,Podio L9ORCID,Schutzer A1,Rivera-Ortiz P R1ORCID,Lépine J R D7,Bachiller R10

Affiliation:

1. CNRS, IPAG, Univ. Grenoble Alpes, F-38000 Grenoble, France

2. Institut de Ciéncies de l’Espai (ICE, CSIC), Can Magrans, s/n, E-08193 Cerdanyola del Vallés, Catalonia, Spain

3. Institut d’Estudis Espacials de Catalunya (IEEC), E-08034 Barcelona, Catalonia, Spain

4. Leiden Observatory, Leiden University, PO Box 9513, NL-2300 RA Leiden, the Netherlands

5. Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, England

6. IRAP, CNRS, UPS, CNES, Université de Toulouse, F-31400 Toulouse, France

7. Instituto de Astronomia, Geofísica e Ciências Atmosféricas, Universidade de São Paulo, São Paulo 05508-090, SP, Brazil

8. INAF, Istituto di Astrofisica e Planetologia Spaziali, via Fosso del Cavaliere 100, I-00133 Roma, Italy

9. INAF, Osservatorio Astrofisico di Arcetri, Largo Enrico Fermi 5, I-50125 Firenze, Italy

10. IGN, Observatorio Astronómico Nacional, Calle Alfonso XII, 3 E-28004 Madrid, Spain

Abstract

ABSTRACT Hydrogen cyanide (HCN) and its isomer hydrogen isocyanide (HNC) play an important role in molecular cloud chemistry and the formation of more complex molecules. We investigate here the impact of protostellar shocks on the HCN and HNC abundances from high-sensitivity IRAM 30 m observations of the prototypical shock region L1157-B1 and the envelope of the associated Class 0 protostar, as a proxy for the pre-shock gas. The isotopologues H12CN, HN12C, H13CN, HN13C, HC15N, H15NC, DCN, and DNC were all detected towards both regions. Abundances and excitation conditions were obtained from radiative transfer analysis of molecular line emission under the assumption of local thermodynamical equilibrium. In the pre-shock gas, the abundances of the HCN and HNC isotopologues are similar to those encountered in dark clouds, with an HCN/HNC abundance ratio ≈1 for all isotopologues. A strong D-enrichment (D/H ≈ 0.06) is measured in the pre-shock gas. There is no evidence of 15N fractionation neither in the quiescent nor in the shocked gas. At the passage of the shock, the HCN and HNC abundances increase in the gas phase in different manners so that the HCN/HNC relative abundance ratio increases by a factor 20. The gas-grain chemical and shock model uclchem allows us to reproduce the observed trends for a C-type shock with pre-shock density n(H) = $10^5\hbox{cm$^{-3}$}$ and shock velocity $V_\mathrm{ s}= 40\hbox{kms$^{-1}$}$. We conclude that the HCN/HNC variations across the shock are mainly caused by the sputtering of the grain mantle material in relation with the history of the grain ices.

Funder

Labex

French National Research Agency

ERC

Fundação de Amparo à Pesquisa do Estado de São Paulo

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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