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Untitled - Laboratoire d'Astrophysique de l'Observatoire de Grenoble

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et al. 2002, 2003). When CO disappears from the gas phase (because con<strong>de</strong>nsed onto the grain mantles),<br />

ratio is highly enhanced and can reach the unity (Caselli et al. 2003). Besi<strong>de</strong>s, even the<br />

the H2D + /H + 3<br />

multiple <strong>de</strong>uterated forms of H + 3 , namely HD+ 2 and D+ 3 , can become more abundant than H+ 3 (Roberts,<br />

Herbst & Millar 2003, ApJ 591, L41). Since the <strong>de</strong>uterated forms of H + 3 react with all molecules in the<br />

gas phase exchanging the D atom, they transmit the <strong>de</strong>uteration to molecules (e.g. Roberts, Herbst &<br />

Millar 2004, A&A 424, 905).<br />

• Molecules like H2CO, CH3OH and H2S, which are thought to form on the grain surfaces rather than in<br />

the gas phase, have been found to show up the largest multiple <strong>de</strong>uteration factors (Parise et al. 2002,<br />

2004a; Vastel et al. 2003). Very likely this is because they are formed by hydrogenation of CO (and S)<br />

during the last phases of the pre-collapse, when the CO <strong>de</strong>pletion is larger (this is a <strong>de</strong>finition!).<br />

• Water though does not follow the same route. In<strong>de</strong>ed, the gaseous HDO/H2O ratio is less than 3% in low<br />

mass protostars (Parise et al. 2005), whereas HDCO/H2CO and CH2DOH/CH3OH ratios are around<br />

30%. Even the solid HDO/H2O ratio is in<strong>de</strong>ed less than 3% (Parise et al. 2004b), which confirms the<br />

lower <strong>de</strong>uteration of water. One possible interpretation is that water forms on the grain surfaces at an<br />

higher temperature, because the H2O con<strong>de</strong>nsation occurs already at about 100 K. This would limit the<br />

H2D + /H + 3 ratio.<br />

• At the center of the Pre-Stellar Cores, all CO is now believed to almost completely freeze-out onto the<br />

grain mantles. Therefore, CO and all the other heavy-bearing molecules disappear from the gas phase,<br />

and the best tool to probe those regions is the H2D + emission (Caselli et al. 2003). The study of the<br />

profile of the H2D + ground state transition provi<strong>de</strong>s a valuable tool to probe the velocity field at the<br />

center of the con<strong>de</strong>nsation, and, consequently, whether and how the collapse sets in (van <strong>de</strong>r Tak, Caselli<br />

& Ceccarelli 2005).<br />

• Similarly to the centers of the Pre-Stellar Cores, the gas in the midplane of the proto-planetary disks<br />

surrounding solar type protostars can only be probed by the H2D + emission (Ceccarelli et al. 2004,<br />

Ceccarelli & Dominik 2005). This aspect will be discussed in more <strong>de</strong>tail in §3.5.<br />

3.2.3 The hot corinos of solar type protostars<br />

In the first phases of the star birth, the future star is embed<strong>de</strong>d in and totally obscured by the infalling material,<br />

which forms a thick envelope. The <strong>de</strong>nsity in the envelope ranges between 10 4 to 10 8 cm −3 , and the temperature<br />

ranges between 10 and about 200 K. The exact <strong>de</strong>nsity and temperature structure <strong>de</strong>pends on the dynamics of<br />

the collapse. It is therefore extreme important to study the <strong>de</strong>nsity and temperature profiles of these envelopes<br />

and how they evolve with time. Furthermore, giving the involved <strong>de</strong>nsities and temperatures, protostellar<br />

envelopes are privileged sites for a rich chemistry to occur. The chemical composition of these envelopes is<br />

not only interesting in itself. The matter in protostellar envelopes forms the proto-planetary disks, which will<br />

eventually form the planets and comets. During the comets bombarding phase, molecules formed during the<br />

protostellar collapse phase may be preserved ( for example frozen-out onto the dust grains) and brought to<br />

the formed planets. It is therefore of paramount importance to know the molecular complexity reached in the<br />

protostellar envelopes. In this context, Astromol members, in collaboration with WAGOS, have contributed to<br />

three major aspects:<br />

• The study of the physical structure. Astromol members published the very first articles reconstructing<br />

the <strong>de</strong>nsity and temperature profiles of protostellar envelopes ( Ceccarelli et al. 2000 A&A 355, 1129;<br />

2000 A&A 357, L9; 2001 A&A 372, 998; Maret et al. 2002, 2004, 2005). Based on these studies, the<br />

protostellar envelopes have approximatively the structure of free-infalling envelopes, as predicted by the<br />

insi<strong>de</strong>-out theory by Shu and colleagues. In addition, they possess warm and <strong>de</strong>nse regions close to the<br />

central object where the icy grain mantles sublimate, injecting into the gas phase the molecules formed<br />

and/or trapped into the mantles.<br />

• The study of the chemical composition. Chemically, the protostellar envelopes are formed by two components:<br />

i) an outer envelope (<strong>de</strong>fined by where the dust temperature is less than ∼ 100 K), whose chemical<br />

composition is similar to that in molecular clouds; ii) an inner envelope, where the chemistry is dominated<br />

by the material sublimated from the icy grain mantles. In this inner envelopes, large quantities of H2O,<br />

H2CO, CH3OH, SO and SO2 molecules are found (Maret et al. 2002, 2004, 2005; Wakelam et al. 2004a,<br />

2004b).<br />

51

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