Evolution of the Outgassing of Comet Hale-Bopp (C/1995 O1) from Radio Observations

Author:

Biver Nicolas1,Bockelée-Morvan Dominique1,Colom Pierre1,Crovisier Jacques1,Davies John K.2,Dent William R. F.2,Despois Didier3,Gérard Eric1,Lellouch Emmanuel1,Rauer Heike1,Moreno Raphael1,Paubert Gabriel1

Affiliation:

1. N. Biver, D. Bockelée-Morvan, P. Colom, J. Crovisier, E. Gérard, E. Lellouch, H. Rauer, Observatoire de Paris-Meudon, F-92195 Meudon, France.

2. J. K. Davies and W. R. F. Dent, Joint Astronomy Centre, 660 North A'ohoku Place, University Park, Hilo, HI 96720-6030, USA.

3. D. Despois, Observatoire de Bordeaux, B.P. 89, F-33270 Floirac, France. R. Moreno and G. Paubert, Institut de Radioastronomie Millimétrique, Avenida Divina Pastora 7, 18012 Granada, Spain.

Abstract

Spectra obtained from ground-based radio telescopes show the progressive release of CO, CH 3 OH, HCN, H 2 O (from OH), H 2 S, CS, H 2 CO, CH 3 CN, and HNC as comet Hale-Bopp (C/1995 O1) approached the sun from 6.9 to 1.4 astronomical units (AU). The more volatile species were relatively more abundant in the coma far from the sun, but there was no direct correlation between overabundance and volatility. Evidence for H 2 O sublimation from icy grains was seen beyond 3.5 AU from the sun. The change from a CO-driven coma to an H 2 O-driven coma occurred at about 3 AU. The gas outflow velocity and temperature increased as Hale-Bopp approached the sun.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference42 articles.

1. Bockelée-Morvan D., Molecules in Astrophysics: Probes and Processes, , van Dishoeck E., Ed. (IAU Symp. 178, Kluwer Academic, Dordrecht, Netherlands)in press.

2. Senay M. C., Jewitt D., Nature 371, 229 (1994);

3. Crovisier J., et al., Icarus 115, 213 (1995).

4. Hale A. Bopp T. IAU Circular 6187 (1995).

5. The half-power beam width (HPBW) of the IRAM antenna is 10 arc sec at 230 GHz and 26 arc sec at 89 GHz. Most of the spectra were acquired at a spectral resolution of 20 to 40 kHz corresponding to velocities of 0.026 to 0.052 km s −1 at 230 GHz. Whenever possible a frequency-switching mode was used.

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