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CO in absorption and emission toward compact extragalactic radio continuum sources

H. S. Liszt tex2html_wrap_inline1123 and R. Lucas tex2html_wrap_inline1115 .
tex2html_wrap_inline1123 NRAO, 520 Edgemont Road, Charlottesville, VA, USA 22903-2475
tex2html_wrap_inline1115 IRAM, 300 Rue de la Piscine, F-38406 Saint Martin d'Hères, France
Abstract: We have observed galactic tex2html_wrap_inline1023 2.6mm and tex2html_wrap_inline1023 1.3mm CO absorption and emission along nine lines of sight toward compact extragalactic mm-wave continuum sources, using the IRAM Plateau de Bure Interferometer and NRAO 12m telescopes. In absorption we detected some two dozen kinematic components, and nearly every feature known from HCO tex2html_wrap_inline1255 spectra has a direct CO counterpart: a few CO lines are missing or very weak in emission even when tex2html_wrap_inline1257 . The column densities of CO and HCO tex2html_wrap_inline1255 are well correlated, but not linearly related. The widths of the CO lines are typically 15% smaller than those of HCO tex2html_wrap_inline1255 (on average 0.75 kms tex2html_wrap_inline1027 vs. 0.86 kms tex2html_wrap_inline1027 ).

We derive tex2html_wrap_inline1151 CO column densities tex2html_wrap_inline1271 which are in all cases very small compared to the column of carbon nuclei expected for 1 magnitude of visual extinction, even allowing for substantial depletion. The partial thermal pressure of tex2html_wrap_inline1273 is inferred to be tex2html_wrap_inline1275 K, with a median p/k = tex2html_wrap_inline1277 K. Thus the clouds are likely warm ( tex2html_wrap_inline1279 tens of K), somewhat diffuse ( tex2html_wrap_inline1281 ), with the majority of the gas-phase carbon in the form of C tex2html_wrap_inline1255 and perhaps even with a substantial fraction of H I in the thinnest cases.

The isotope ratios in the CO usually differ strongly from the local interstellar ratio which we have separately measured in these clouds to be tex2html_wrap_inline1151 C/ tex2html_wrap_inline1019 C = 60 ; we find tex2html_wrap_inline1289 N tex2html_wrap_inline1291 N tex2html_wrap_inline1293 , declining with increasing N( tex2html_wrap_inline1151 CO). The tex2html_wrap_inline1019 CO/C tex2html_wrap_inline1301 O ratio seen in emission or absorption is typically 25 (instead of 8) and C tex2html_wrap_inline1301 O is very difficult to detect in emission even when tex2html_wrap_inline1305 . Apparently, the relative abundance of tex2html_wrap_inline1019 CO is typically greatly enhanced, even at very low extinction, and never diminished by selective photodissociation. One effect of this enhancement is that lines of tex2html_wrap_inline1151 CO are substantially less optically thick than might otherwise have been inferred. There is little evidence for a general selective depletion of C tex2html_wrap_inline1301 O.

Preprint requests: lucas@iram.fr


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Next: Physical parameters of the Up: Scientific results Previous: CO at the centre

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