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

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Differential Cross Section (Å 2 sr -1 )<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

0 20 40 60 80 100 120 140 160 180<br />

Scattering Angle (<strong>de</strong>g)<br />

Figure 3.6: Computed and measured DCS of water at 6 eV. The present elastic (rotationally summed) DCS<br />

is given by the thick solid line. Other lines <strong>de</strong>note partial state-to-state DCS (dashed line: 0 → 1; solid line:<br />

0 → 0). The filled squares correspond to the experimental elastic DCS of (Cho et al. 2004 J. Phys. B, 37<br />

4639). The open circles and diamonds correspond respectively to the experimental pure elastic (∆j = 0) and<br />

rotationally inelastic (∆j = ±1) DCS of (Jung et al. 1982 J. Phys. B, 15 3535); the sum of both contributions<br />

is given by the stars. Taken from Gorfinkiel et al. (2005 Eur. Phys. J. D, 35, 231).<br />

3.4 High Performance Computing<br />

The Astromol team has been involved in several high performance computing initiatives to achieve its objectives.<br />

The most <strong>de</strong>manding issue was the construction of multi-dimensional ab-initio potential energy surfaces and their<br />

calibration to cm −1 accuracy using our explicitely correlated coupled cluster approach. The inelastic scattering<br />

calculations proved also very <strong>de</strong>manding, both at the classical level (to investigate the H2O quenching) and at<br />

the close coupling level (CO colliding with H2 and HC3N colliding with He and H2). In the future, exploration<br />

of multi-parametric mo<strong>de</strong>ls of astrophysical sources may also prove very <strong>de</strong>manding, as was already explored<br />

by S. Maret.<br />

In or<strong>de</strong>r to achieve our goals at optimal cost, we combined a hierarchy of approaches and machines.<br />

• Our <strong>de</strong>velopment benefited of a few <strong>de</strong>dicated PCs acquired with support of PCMI and CNES, and<br />

complemented at the end of 2004 by a 64-bit opteron biprocessor with 8 GB memory which was <strong>de</strong>voted<br />

to explicitely correlated investigations. This latter machine was also used as a testbed for the preparation<br />

of the invitation to ten<strong>de</strong>r for the upgra<strong>de</strong> of the computing center of the Observatory (see below).<br />

• Large ab-initio production calculations, either conventional or explicitely correlated, were run on the<br />

national supercomputers. We submitted a huge <strong>de</strong>mand in 2005 to boost the calculations of all the<br />

potential energy surfaces related to the “Molecular Universe” FP6 project. We obtained 60000 hours on<br />

the IDRIS and the CEA supercomputers and 100000 hours on the CINES.<br />

• Multi-dimensional potential energy surfaces were sampled by a multi-parametric Monte Carlo procedure.<br />

The 9-D surface for H2O-H2 required 375000 in<strong>de</strong>pen<strong>de</strong>nt geometries, each combining a counterpoise of<br />

3 ab-initio calculations resulting into over a million of short ab-initio runs. This computational challenge<br />

triggered a pluri-disciplinary <strong>de</strong>velopment of the <strong>Grenoble</strong> computer grid “CiGri” with the support of<br />

a 3-year CDD fun<strong>de</strong>d by the ACI GRID and a strong involvment of the STIC community (INRIA and<br />

IMAG). A CiGrid protopype permitted to gather about 200000 cpu hours on idle PCs and to achieve the<br />

9-D surface for H2O-H2 within two months. Presently CiGri matured to a convivial middleware, and has<br />

been used for classical scattering calculations in our team and by other projects (including optimisation<br />

studies for the MARSIS sub-surface radar observations on Mars Express).<br />

61

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