Seven rotational transitions of SiC 3 , a planar, highly polar ring molecule, have been detected in the millimeterwave band in the expanding envelope of the evolved carbon star IRC ϩ10216. On the assumption that SiC 3 has the same 40Љ diameter shell as SiCC, the mean column density of SiC 3 is cm . The rotational 12 Ϫ24.3 # 10 excitation of SiC 3 is similar to that of SiCC, with a low rotational temperature within the K-stacks of 10-20 K and a high rotational temperature across the K-stacks of roughly 50 K, which is probably close to the kinetic temperature of the shell.Subject headings: ISM: molecules -line: identification -molecular data -molecular processesradio lines: ISMThe most stable molecule with the elemental formula SiC 3 has been calculated to be the rhomboidal isomer with a transannular bond, as shown in Figure 1 (Alberts, Grev, & Schaefer 1990;Gomei et al. 1997). It has recently been detected for the first time in this laboratory, and its rotational spectrum has been measured to high precision in both the centimeterand millimeter-wave bands Apponi et al. 1999). Observing at the laboratory frequencies, we have now detected, with the NRAO 3 12 m telescope on Kitt Peak, seven transitions of this unusual molecular ring in the rich molecular envelope of the evolved carbon star IRC ϩ10216, which is a source where three silicon-carbon molecules have already been detected: the diatomic radical SiC al. 1997], the only stable ring so far detected).The observations are summarized in Table 1, and four of the lines are shown in Figure 2. The uncertainties in our rest frequencies are only 0.3 km s or less and, therefore, negligible Ϫ1 relative to both the width of the lines in the molecular shell of IRC ϩ10216 (28 km s ) and the spectral resolution of our Ϫ1 observations (3-4 km s ). Lines of nearly all molecules in Ϫ1 this source lie at a radial velocity of Ϫ km s , which,
Ϫ126 ע 1 as Table 1 shows, to within the observational uncertainties, is the velocity of all the lines attributed to SiC 3 . Because the average interval between unidentified lines as strong as 5 mK in this part of the spectrum of IRC ϩ10216 is at least 30 MHz in frequency, or 100 km s in velocity, the probability that Ϫ1 any one of our seven lines is misidentified is a few percent at most, and the joint probability that all are misidentified is extremely small. In spite of its fairly weak lines, is one of the more securely identified molecules in IRC ϩ10216.The observations were done with the 12 m NRAO telescope on Kitt Peak during 1998 December when the sky was clear and the zenith opacity of water vapor at 225 GHz was generally 0.2 or less. The dual polarization SIS receiver used for the observations had a single-sideband system temperature of 200 K or less, atmospheric emission included. Pointing was checked every few hours against Saturn or 3C 273 and was found to be good to 10Љ. Spectra were taken by beam switching with the telescope's nutating subreflector at 1.25 Hz, with an angular throw of 4Ј. Two filter banks, each of 256...