13.07.2015 Views

[tel-00726959, v1] Caractériser le milieu interstellaire ... - HAL - INRIA

[tel-00726959, v1] Caractériser le milieu interstellaire ... - HAL - INRIA

[tel-00726959, v1] Caractériser le milieu interstellaire ... - HAL - INRIA

SHOW MORE
SHOW LESS
  • No tags were found...

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

A&A 534, A49 (2011)<strong>tel</strong>-<strong>00726959</strong>, version 1 - 31 Aug 2012Tab<strong>le</strong> 5. Column densities and abundances.Column densities[cm −2 ]Abundances[X] =N(X)(N(H)+2 N(H 2 ))Mo<strong>le</strong>cu<strong>le</strong> PDR Dense-coreN H 3.8 × 10 22 6.4 × 10 22N(o-H 2 CO) 7.2 × 10 12 9.6 × 10 12N(p-H 2 CO) 3.6 × 10 12 3.2 × 10 12N(HCO) a 3.2 × 10 13 50 K), so the deuterium chemistry is drivenmainly by CH 2 D + , as opposed to colder regions (20 K) like theHorsehead dense-core, where H 2 D + is the main actor. Owing tothe low temperature in the core it is likely that a non-negligib<strong>le</strong>fraction of CO is frozen on the dust grains, enhancing the deuteriumfractionation.Another way to form deuterated mo<strong>le</strong>cu<strong>le</strong>s in cold environmentsis trough D addition or H-D substitution reactions on thesurface of dust grains (Hidaka et al. 2009). In the Horsehead corethough, desorption from the grain mant<strong>le</strong>s is not efficient in re<strong>le</strong>asingproducts into the gas-phase (see Sect. 4). It is then morelikely that the gas-phase HDCO and D 2 CO mo<strong>le</strong>cu<strong>le</strong>s detectedhere are formed in the gas-phase. Neverthe<strong>le</strong>ss, there can still bea considerab<strong>le</strong> amount of deuterated H 2 CO trapped in the icesaround dust grains.4. H 2 CO chemistryWe used a one-dimensional, steady-state photochemical model(Le Bourlot et al. 1993; Le Petit et al. 2006) to study the H 2 COchemistry in the Horsehead. The physical conditions have alreadybeen constrained by our previous observational studiesand we keep the same assumptions for the density profi<strong>le</strong> (displayedin the upper panel of Fig. 6), radiation field (χ = 60in Draine units), e<strong>le</strong>mental gas-phase abundances (see Tab<strong>le</strong> 6in Goicoechea et al. 2009b) and cosmic ray ionization rate(ζ = 5 × 10 −17 s −1 ).Unlike other organic mo<strong>le</strong>cu<strong>le</strong>s like methanol, which canonly be efficiently formed on the surface of grains (Tie<strong>le</strong>ns &Whittet 1997; Woon 2002; Cuppen et al. 2009), formaldehydecan be formed in both the gas-phase and on the surface of grains.Next, we investigate these two different scenarios.4.1. Pure gas-phase chemistry modelsWe used the Ohio State University (osu) pure gas-phase chemicalnetwork upgraded to photochemical studies. We included the

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!