H 2 , H 3 + and the age of molecular clouds and prestellar cores

Author:

Pagani L.1,Lesaffre P.2,Roueff E.3,Jorfi M.4,Honvault P.56,González-Lezana T.7,Faure A.8

Affiliation:

1. LERMA, UMR8112 du CNRS, Observatoire de Paris, 61, Av. de l'Observatoire, 75014 Paris, France

2. LERMA, UMR8112 du CNRS, Ecole Normale Supérieure, 24 rue Lhomond, 75231 Paris Cedex 05, France

3. LUTh, UMR8102 du CNRS, Observatoire de Paris, 5, place Jules Janssen, 92195 Meudon Cedex, France

4. Laboratoire de Catalyse en Chimie Organique, UMR CNRS 6503, Université de Poitiers, 86022 Poitiers Cedex, France

5. Laboratoire Interdisciplinaire Carnot de Bourgogne, UMR 5209 du CNRS, Université de Bourgogne, 21078 Dijon Cedex, France

6. UFR Sciences et Techniques, Université de Franche-Comté, 25030 Besançon Cedex, France

7. Instituto de Física Fundamental, CSIC, Serrano 123, 28006 Madrid, Spain

8. Institut de Planétologie et d'Astrophysique de Grenoble, UMR 5274 du CNRS, Université Joseph Fourier, BP 53, 38041 Grenoble Cedex 09, France

Abstract

Measuring the age of molecular clouds and prestellar cores is a difficult task that has not yet been successfully accomplished although the information is of paramount importance to help in understanding and discriminating between different formation scenarios. Most chemical clocks suffer from unknown initial conditions and are therefore difficult to use. We propose a new approach based on a subset of deuterium chemistry that takes place in the gas phase and for which initial conditions are relatively well known. It relies primarily on the conversion of H 3 + into H 2 D + to initiate deuterium enrichment of the molecular gas. This conversion is controlled by the ortho/para ratio of H 2 that is thought to be produced with the statistical ratio of 3 and subsequently slowly decays to an almost pure para-H 2 phase. This slow decay takes approximately 1 Myr and allows us to set an upper limit on the age of molecular clouds. The deuterium enrichment of the core takes longer to reach equilibrium and allows us to estimate the time necessary to form a dense prestellar core, i.e. the last step before the collapse of the core into a protostar. We find that the observed abundance and distribution of DCO + and N 2 D + argue against quasi-static core formation and favour dynamical formation on time scales of less than 1 Myr. Another consequence is that ortho-H 2 remains comparable to para-H 2 in abundance outside the dense cores.

Publisher

The Royal Society

Subject

General Physics and Astronomy,General Engineering,General Mathematics

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