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

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

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A&A 534, A49 (2011)DOI: 10.1051/0004-6361/201117257c○ ESO 2011Astronomy&AstrophysicsH 2 CO in the Horsehead PDR:photo-desorption of dust grain ice mant<strong>le</strong>sV. Guzmán 1,2 ,J.Pety 2,1 , J. R. Goicoechea 3 , M. Gerin 1 , and E. Roueff 41 LERMA – LRA, UMR 8112, Observatoire de Paris and Éco<strong>le</strong> Norma<strong>le</strong> Supérieure, 24 rue Lhomond, 75231 Paris, Francee-mail: [viviana.guzman;maryvonne.gerin]@lra.ens.fr2 IRAM, 300 rue de la Piscine, 38406 Grenob<strong>le</strong> Cedex, Francee-mail: pety@iram.fr3 Departamento de Astrofísica, Centro de Astrobiología, CSIC-INTA, Carretera de Ajalvir, Km 4, Torrejón de Ardoz,28850 Madrid, Spaine-mail: jr.goicoechea@cab.inta-csic.es4 LUTH UMR 8102, CNRS and Observatoire de Paris, Place J. Janssen, 92195 Meudon Cedex, Francee-mail: evelyne.roueff@obspm.frReceived 13 May 2011 / Accepted 22 August 2011<strong>tel</strong>-<strong>00726959</strong>, version 1 - 31 Aug 2012ABSTRACTAims. For the first time we investigate the ro<strong>le</strong> of the grain surface chemistry in the Horsehead photo-dissociation region (PDR).Methods. We performed deep observations of several H 2 CO rotational lines toward the PDR and its associated dense-core in theHorsehead nebula, where the dust is cold (T dust ≃ 20−30 K). We comp<strong>le</strong>mented these observations with a map of the p-H 2 CO 3 03 −2 02line at 218.2 GHz (with 12 ′′ angular resolution). We determine the H 2 CO abundances using a detai<strong>le</strong>d radiative transfer analysis andcompare these results with PDR models that include either pure gas-phase chemistry or both gas-phase and grain surface chemistry.Results. The H 2 CO abundances (≃2–3 × 10 −10 ) with respect to H-nuc<strong>le</strong>i are similar in the PDR and dense-core. In the dense-core thepure gas-phase chemistry model reproduces the observed H 2 CO abundance. Thus, surface processes do not contribute significantly tothe gas-phase H 2 CO abundance in the core. In contrast, the formation of H 2 CO on the surface of dust grains and subsequent photodesorptioninto the gas-phase are needed in the PDR to explain the observed gas-phase H 2 CO abundance, because the gas-phasechemistry alone does not produce enough H 2 CO. The assignments of different formation routes are strengthen by the different measuredortho-to-para ratio of H 2 CO: the dense-core displays the equilibrium value (∼3) whi<strong>le</strong> the PDR displays an out-of-equilibriumvalue (∼2).Conclusions. Photo-desorption of H 2 CO ices is an efficient mechanism to re<strong>le</strong>ase a significant amount of gas-phase H 2 CO into theHorsehead PDR.Key words. astrochemistry – ISM: clouds – ISM: mo<strong>le</strong>cu<strong>le</strong>s – ISM: individual objects: Horsehead nebula – radiative transfer –radio lines: ISM1. IntroductionPhoto-dissociation region (PDR) models are used to understandthe evolution of the far-UV illuminated matter both in ourGalaxy and in external galaxies. The spectacular instrumentalimprovements, which happen in radioastronomy with the adventof Herschel, ALMA and NOEMA, call for matching progressesin PDR modeling. In particular, the physics and chemistry of thedust grains and of the gas-phase are intrica<strong>tel</strong>y intertwined. It iswell known that the formation of ice grain mant<strong>le</strong>s <strong>le</strong>ads to theremoval of chemical reservoirs like CO, O, and other abundantspecies from the gas phase, enabling new chemical routes to beopened and others to be closed. Despite their low temperature,the mant<strong>le</strong>s are chemically active. Hydrogenation/deuterationreactionsare known to be efficient, because hydrogen (or deuteriumatoms) can migrate on the surfaces, but reactions withO, N, and C must also be considered. Comp<strong>le</strong>x mo<strong>le</strong>cu<strong>le</strong>s maytherefore be formed before they are re<strong>le</strong>ased into the gas phase.Moreover, the re<strong>le</strong>ase of the products into the gas phase happenseither through thermal processes (evaporation) or non-thermalones (cosmic ray or far-UV photon-induced desorption). Recentphoto-desorption experiments on water and CO ices show thatthis mechanism is much more efficient than previously thought(Öberg et al. 2009b,a; Muñoz Caro et al. 2010). These results<strong>le</strong>d various groups to include photo-desorption into PDR models(see the results on H 2 OandO 2 by Hol<strong>le</strong>nbach et al. 2009; Walshet al. 2010; Hassel et al. 2010). The availability of well-definedobservations is essential here to distinguish between chemicalassumptions about the significant grain surface processes, i.e.,adsorption, desorption, and diffusion. It is now confirmed thatsome inters<strong>tel</strong>lar species are mostly formed in the gas-phase (COfor instance), others on grains (CH 3 OH, Garrod et al. 2007),whi<strong>le</strong> the chemical routes for other comp<strong>le</strong>x species such asformaldehyde, are still debated because it is likely that solid andgas-phase processes are both needed.Formaldehyde (H 2 CO) was the first organic mo<strong>le</strong>cu<strong>le</strong> discoveredin the inters<strong>tel</strong>lar medium (Snyder et al. 1969). It is arelatively simp<strong>le</strong> organic mo<strong>le</strong>cu<strong>le</strong> that can be formed in the gasphaseand on the surface of dust grains. In the warm gas, H 2 COcan trigger the formation of more comp<strong>le</strong>x organic mo<strong>le</strong>cu<strong>le</strong>s(Charn<strong>le</strong>y et al. 1992). It is one of the most popular mo<strong>le</strong>cu<strong>le</strong>sused for studying the physical conditions of the gas in astrophysicalsources. Indeed, it is a good probe of the temperatureand density of the gas (Mangum & Wootten 1993). Owing to itsArtic<strong>le</strong> published by EDP Sciences A49, page 1 of 9

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