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4. CHEMICAL PROCESSING

Just as modeling of stellar atmospheres is important, we are also beginning to pursue models of interstellar clouds. We need to gain a better understanding of chemical processes and the spectra that would identify them as interstellar clouds collapse, are shocked, form new molecular species, or are lit up by the formation of a new star. We can test such models of chemical networks against spectra ISO is now providing.

A most useful tool for studying a variety of gaseous domains is the CLOUDY program of Gary Ferland. His collaborator, Peter van Hoof, displayed how this program facilitates the study of photodissociation regions (PDRs)and starburst galaxies. Both Frank Bertoldi and Pierre Cox showed us the information that now can be derived for PDRs. In particular, a large number of rovibrational emission lines of molecular hydrogen H tex2html_wrap_inline84 are clearly discerned. If we select only the rotational transitions of the ground vibrational state, we can plot the excitation energy of a given rotational state J against observed column densities N(J) divided by statistical weight g(J)= n(2J+1). Here n = 3 for ortho and 1 for para states, respectively the odd and even angular momentum states including J = 0. The slopes of these plots for the PDRs in S140 and NGC 7023 reveal surprisingly high temperatures, respectively, 500 and 580K.

In the planetary nebular NGC 7027 Xiaowei Liu showed us spectral features of CH tex2html_wrap_inline148 that he, José Cernicharo and coworkers had identified. Once again, long-available laboratory spectra permitted this identification. Unidentified lines in this and other planetary nebulae, however, persist and may arise from unknown molecular species.

A poster by Paolo Saraceno and coworkers showed water vapor emission to be unexpectedly low in shocked interstellar regions. They found water vapor cooling to be typically an order of magnitude or more lower than cooling through CO transitions. Saraceno feels that water vapor may be under abundant in these regions. If so, this raises another problem. In the sun oxygen is roughly twice as abundant as carbon. We speak of a cosmic abundance of oxygen which is roughly twice that of carbon. In interstellar clouds the abundance of oxygen appears to be anomalously low. By now we have the ability to observe oxygen in its atomic form and as OH, as H tex2html_wrap_inline84 O ice and vapor, as CO, and as CO tex2html_wrap_inline84 . Carbon is present in atomic form and as CO, CO tex2html_wrap_inline84 , CH tex2html_wrap_inline86 and larger organic molecules, and perhaps as graphite in grains. This makes it difficult to see an abundance of oxygen that might still be twice as high as that of carbon, unless oxygen was present in molecular form, O tex2html_wrap_inline84 . But this may already be ruled out by the apparent absence of solid O tex2html_wrap_inline84 in ices. Laboratory spectra of ices consisting of H tex2html_wrap_inline84 O, CO, and CO tex2html_wrap_inline84 show changes in shape when O tex2html_wrap_inline84 is admixed. Pascale Ehrenfreund told us that such features are not found in the spectra of interstellar ices, suggesting that O tex2html_wrap_inline84 is not a significant component. Searches with ISO for gaseous O tex2html_wrap_inline84 are also being carried out. It will be interesting to see what they will teach us. Molecular oxygen is difficult to observe because of its symmetric dipole structure, and we may not be able to put significant upper limits on its abundance. The interstellar abundance of oxygen is one of the log-standing problems of interstellar chemistry that ISO may still have an opportunity to clarify.


next up previous
Next: 5. GALAXIES Up: REVIEW OF THE WORKSHOP Previous: 3. THE IMPORTANCE OF

Martin Harwit

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