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Chemical inhomogeneities in interstellar clouds: The high latitude cloud MCLD 123.5+24.9

M. Gerin tex2html_wrap_inline1476 , E. Falgarone tex2html_wrap_inline1478 , K. Joulain tex2html_wrap_inline1480 , M. Kopp tex2html_wrap_inline1482 , J. Le Bourlot tex2html_wrap_inline1484 , G. Pineau des Forêts tex2html_wrap_inline1486 , E. Roueff tex2html_wrap_inline1488 , P. Schilke tex2html_wrap_inline1490
tex2html_wrap_inline1492 Downs Laboratory of Physics, Caltech, Physics Department, 320-47, Pasadena CA91125, USA.
tex2html_wrap_inline1494 Radioastronomie Millimétrique, Laboratoire de Physique de l'ENS, 24 rue Lhomond, 75231 Paris Cedex 05, France
tex2html_wrap_inline1496 DAEC, Observatoire de Paris-Meudon, Place J. Janssen, 92195 Meudon cedex, France
tex2html_wrap_inline1498 I. Physikalisches Institut der Universität zu Köln, Zülpicher Str. 77, D-50937, Köln, Germany
Abstract: We report on observations designed to disclose the presence of the High Ionization Phase predicted to exist in dark clouds by chemical models (Le Bourlot et al., 1993). In addition to a high neutral carbon abundance, a high CS/SO abundance ratio and a low abundance of molecular ions, such a phase might be characterized by a low D/H fractionation ratio.
In this paper, we present both observational and model results on the sulfur bearing molecules CS and SO, and their most abundant isotopomers, on the molecular ions tex2html_wrap_inline1500 , tex2html_wrap_inline1502 , tex2html_wrap_inline1504 and tex2html_wrap_inline1506 . We have also taken new tex2html_wrap_inline1508 and tex2html_wrap_inline1510 data to improve the determination of the physical conditions at the observed positions. One of the two dark clouds investigated, a core in the high latitude cloud MCLD 123.5+24.9, presents surprinsingly strong CS and tex2html_wrap_inline1512 lines relative to its column density, together with weak tex2html_wrap_inline1514 lines. It has also a cold temperature and rather strong CCH and C tex2html_wrap_inline1516 H tex2html_wrap_inline1518 lines. These observed features are characteristic of the presence of the High Ionization Phase along the line of sight. This cloud core might therefore be a good candidate for further investigation of this new phase of dark interstellar clouds.

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Figure 3: Column density ratio N(CS)/N(SO) as a function of the tex2html_wrap_inline1520 column density for Polaris (black squares), Taurus (black triangles), TMC1 (asterisks), L134N (crosses), B335 (white square), clouds seen in absorption (white triangles), dark clouds cores (white hexagons), high latitude clouds (starred squares) and globules (stars).


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