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Astron. Astrophys. 329, 443-450 (1998) 1. IntroductionIsotope ratios derived from CNO elements have significantly contributed to our understanding of the nuclear processing in stars and the 'chemical' evolution of galaxies, since these elements are abundant and have stable 'primary' and 'secondary' nuclei. From a theoretical point of view, 12C/13C is the least controversial CNO isotope ratio: 12C is a 'primary' product of helium-burning, 13C is mainly a 'secondary' product of hydrogen-burning with 12C as the seed nucleus. Some primary 13C may also be synthesized during the third dredge up in stars of intermediate mass ('hot bottom burning', e.g. Renzini & Voli 1981). There is evidence for high 12C/13C
ratios in the central regions of active star-forming galaxies with
high luminosities in the far infrared (for a summary, see Henkel &
Mauersberger 1993). First hints were obtained from distant mergers
(being ultraluminous in the infrared) which were showing integrated
I (12CO)/I (
Since two well studied extragalactic sources represent too small a sample for a comparison with the Milky Way, we have extended this list, including M 82 (NGC 3034) and IC 342. These contain powerful far infrared sources in their central regions and show an impressive amount of strong molecular lines (e.g. Henkel et al. 1986, 1991). From our experience with NGC 253, the best limits to the 12C/13C abundance ratio are obtained from the I (12CN)/I (13CN) line intensity ratios. We observed CN not only toward M 82 and IC 342 but also toward the Galactic center region (see Table 1), where the interstellar 12C/13C ratio is known and where isotope ratios deduced from CN can thus be tested. Table 1. Source list © European Southern Observatory (ESO) 1998 Online publication: December 8, 1997 ![]() |