\\ Version: & 1 & & CH3COCH3 \\ Date: & March 2008 & & Acetone gs, \\ Contributor:& B. J. Drouin & &AA, EE, EA, AE \\ & & & \\ Lines Listed: & 61834 & Q(300.0)=&15502961 \\ Freq. (GHz) $<$ & 1000 & Q(225.0)=& 5262424 \\ Max. J: & 70 & Q(150.0)=& 1434525 \\ LOGSTR0= & -10.0 & Q(75.00)=& 134593 \\ LOGSTR1= & -8.0 & Q(37.50)=& 59894 \\ Isotope Corr.: & 0.0 & Q(18.75)=& 21225 \\ Egy. (cm$^{-1}$) $>$& 0.0 & Q(9.375)=& 8247 \\ $\mu_a$ = & & A=&10165.216 \\ $\mu_b$ = & 2.93 & B=& 8515.165 \\ $\mu_c$ = & & C=& 4910.199 \headend The data set used is compiled from Peter, R., Dreizler, H. 1965, Z. Naturforsch., 20a, 301 Vacherand J.M., van Eijck, B.P., Burie, J. Demaison, J. 1986, J. Mol. Spec. 118, 355. Oldag, F., \& Sutter, D. H., 1992, Z. Naturforsch., 47a, 527. White, W.F. 1975, NASA Tech. Note D-7904, 121. Groner P., Albert S., Herbst E., DeLucia F.C., Lovas F.J., Drouin, B.J., Pearson, J.C., (2002) Ap. J. Supp. 142: 145-151. The v designations separate vibrational levels and torsional sub-levels as follows: \begin{table}[h] \begin{tabular*}{\hsize}{@{\extracolsep{\fill}}c|c|c} & v' & v \\ \hline AA & 0 & 0 \\ EE & 0 & 1 \\ EA & 2 & 1 \\ AE & 1 & 1 \\ \end{tabular*} \end{table} Note that the EE and EA states are treated as l-doubling pairs. The lines were fit to a Hamiltonian that included terms up to the sixth power in angular momentum. Dependence on K expected from an IAM treatment was incorporated using both Energy and B+C Fourier series with fixed ratios of sine and cosine terms in $2 \pi \rho_a K /3$. The quality of the fit was, on the average, about 1.6 experimental uncertainty. The EE and EA states have both b and c type lines, while the AA and AE states have only b type lines. The full vibration-torsion-rotation partition function, including corrections for states not included in the compilation, is utilized for this catalog entry. The rotational partitioning is from Groner et al (2002).