tex2html_wrap_inline391CO J = 1tex2html_wrap_inline3930 observations of the Circinus galaxy using the Mopra 22-m radio-telescope

M. Elmouttie, R.F. Haynes, K.L. Jones, PASA, 14 (2), in press.

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Conclusion

Using the facilities at Mopra, we have successfully detected tex2html_wrap_inline391CO (1-0) at 5 different positions in the Circinus galaxy. Our conclusions based on these initial results are as follows:

(a) The nuclear CO distribution has a profile with a FWHM of 550 pc. The peak emission occurs within 20 tex2html_wrap_inline457 of the radio continuum nucleus.

(b) The velocity components at the centre of the galaxy are distributed in a 445 kmstex2html_wrap_inline407 range, indicating rapid rotation of the molecular gas at the centre of the galaxy.

(c) The molecular mass of the Circinus galaxy is at least 7.5 tex2html_wrap_inline411 4.1 tex2html_wrap_inline413 10tex2html_wrap_inline415 Mtex2html_wrap_inline417.

(d) The star forming efficiency of the galaxy is 16 tex2html_wrap_inline411 9 Ltex2html_wrap_inline417Mtex2html_wrap_inline417tex2html_wrap_inline407 .

These results are consistent with a galaxy undergoing an aggressive stage of nuclear star formation. More data with better resolution and sensitivity are needed to map the molecular gas in the outer regions of the Circinus galaxy and to obtain an understanding of how the gas and the spiral structure are related in this active galaxy. Also, high resolution , high sensitivity FIR data are needed to correctly determine which regions in the galaxy are responsible for star formations. This question is particularly interesting for the Circinus galaxy given its unusual radio continuum morphology and strong radio/infra-red nucleus.


Next Section: Acknowledgements
Title/Abstract Page: CO J = 10
Previous Section: Discussion
Contents Page: Volume 14, Number 2

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