4.7 Article

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

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 507, Issue 1, Pages 1034-1046

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stab2134

Keywords

astrochemistry; methods: observational; ISM: abundances; ISM: molecules; ISM: jets and outflows

Funding

  1. Large Program ASAI [012-12]
  2. Labex Osug@2020 (Investissements d'avenir Labex Osug@2020) by the French National Research Agency through 'Origin of Life' project of the Univ. Grenoble-Alpes [ANR10LABX56, ANR-15-IDEX-02]
  3. ERC Horizon 2020 research and innovation programme 'The Dawn of Organic Chemistry' (DOC) [741002]
  4. ERC Horizon 2020 ITN Project 'Astro-Chemistry Origins' (ACO) [811312]
  5. European Research Council (ERC) [MOPPEX 833460]
  6. Brazilian Fundacao de Amparoa Pesquisa do Estado de Sao Paulo (FAPESP) [2014/22095-6, 2015/22254-0]
  7. State Agency for Research (AEI) of the Spanish MCIU [AYA2017-84390-C2-2-R]

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Hydrogen cyanide (HCN) and its isomer hydrogen isocyanide (HNC) play an essential role in molecular cloud chemistry and the formation of complex molecules. This study investigates the impact of protostellar shocks on the abundances of HCN and HNC, finding that the HCN/HNC ratio increases by a factor of 20 during the passage of the shock. The abundances of HCN and HNC isotopologues in the pre-shock gas are similar to those in dark clouds, with a strong D-enrichment observed.
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 LRAM 30m 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 (HCN)-C-12, (HNC)-C-12, (HCN)-C-13, (HNC)-C-13, (HCN)-N-15, (HNC)-N-15, 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 approximate to 1 for all isotopologues. A strong D-enrichment (D/H approximate to 0.06) is measured in the pre-shock gas. There is no evidence of N-15 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) cm(-3) and shock velocity V-s = 40 km s(-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.

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