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

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particular, we calculated a 9D H2O-H2 potential energy surface of unprece<strong>de</strong>nted accuracy and complexity<br />

(Faure et al 2005a). The associated quenching rate for vibrationally excited water has been calculated<br />

using a classical Monte Carlo canonical approach which corrects by more than one or<strong>de</strong>r of magnitu<strong>de</strong><br />

the existing estimations (Faure et al 2005b). These results will lead to a thorough re-interpretation of<br />

vibrationally excited water emission spectra from space.<br />

iv) We have also reconsi<strong>de</strong>red the role of electrons in the collisional excitation of molecules in harsh environments<br />

(PDR’s, planetary nebulae, etc) in collab. with the group of J. Tennyson at UCL. Rotational<br />

transitions with ∆J > 1, which are neglected in pure dipolar approximations, were found to have rate<br />

constants similar or even larger than those with ∆J = 1. Results of astrophysical relevance have been<br />

obtained for H + 2 , CO+ , NO + , HCO + , H + 3 , H3O + , and asymmetric-top isotopologs of water H2O, HDO<br />

and D2O (Faure et al. 2004 and references therein).<br />

3.2 Star Formation<br />

3.2.1 Overview<br />

Astromol members carry out observational and theoretical studies of the star formation process. These cover<br />

low to high mass (§3.2.5) stars, and concern the very first stages represented by the Molecular Clouds and<br />

Pre-Collapse phases to the last phases before the so called Pre-Main-Sequence (PMS) phase, which is a target<br />

of the FOST team research. Specifically, Astromol studies focus on:<br />

• Molecular Clouds, as the nurseries of newly forming stars (§3.2.2, 3.2.6);<br />

• Pre-Stellar Cores, the con<strong>de</strong>nsations just before the collapse sets in ((§3.2.2);<br />

• Class 0 sources, believed to be the youngest known protostars (§3.2.2, 3.2.3, 3.2.6, 3.2.7);<br />

• Class I sources, believed to represent the transition between Class 0 sources and PMS objects (§3.2.2,<br />

3.2.3, 3.2.6, 3.2.7);<br />

• Proto-planetary disks (this part is <strong>de</strong>scribed in §3.5)<br />

• Molecular outflows, the result of the interaction of the material ejected during the Class 0 and Class I<br />

phases with the surrounding Molecular Clouds (§3.2.4).<br />

To study the formation of the stars and how this influences the surroundings, Astromol members use observational<br />

facilities which span the X-ray (§3.2.6) to radio frequency range. In addition, although molecular<br />

spectroscopy is the Astromol privileged tool to study star forming regions, also dust continuum emission and<br />

features (§3.2.7) have been used by the Astromol members. Consequently, a wi<strong>de</strong> range of mo<strong>de</strong>ls is <strong>de</strong>veloped<br />

to interpret such a wi<strong>de</strong> range of observations. The following sections give a brief summary of the Astromol<br />

research in the mentioned fields.<br />

3.2.2 The <strong>de</strong>uteration in the first phases of star formation<br />

Molecular <strong>de</strong>uteration was consi<strong>de</strong>red sort of a solved problem in Astrophysics, until the first <strong>de</strong>tections of<br />

multiply <strong>de</strong>uterated molecules in low mass star forming regions, which showed molecular D/H ratios enhanced<br />

by up to 8 or<strong>de</strong>rs of magnitu<strong>de</strong> with respect to the elemental D/H ratio (Ceccarelli et al. 1998 A&A 338, L43;<br />

2001 A&A 372, 998; 2002 A&A 381, L17; Loinard et al. 2000 A&A 359, 1169; 2001 ApJ 552, L173). The<br />

current mo<strong>de</strong>ls were unable to fully explain those observations (e.g. Roberts & Millar 2002, A&A 361, 388).<br />

Astromol observational work in the 2002-2005 period has helped to solve the problem, which now is much better<br />

mastered. Specifically, the following aspects were elucidated:<br />

• The extreme <strong>de</strong>uteration observed in low mass protostars sets on during the pre-collapse phase, when the<br />

matter is very <strong>de</strong>nse (≥ 10 6 cm −3 ) and cold (≤ 10 K). This is in the so called Pre-Stellar-Core phase. A<br />

key factor which makes the <strong>de</strong>uteration so extreme is the CO freeze-out onto the grain mantles (Bacmann<br />

50

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