“…Because the rotational constants for acetone-18 O [3], -1,3-( 13 C) 2 [3], -d 6 [5,6], -d 1 [6], and -d 5 [6] were either reported without standard errors or determined for representations other than I r , Table 1 Measured and assigned transition frequencies m obs (MHz), experimental uncertainties Unc. (kHz), and residuals Dm (kHz) of the least-squares fit [3], and -d 6 [5,6], the effective rotational Hamiltonian was the same as the one used for normal acetone and acetone-2-13 C. For the symmetric forms of acetone-d 1 and -d 5 , the effective Hamiltonian used for acetone-1-13 C was modified by setting all parameters pertaining to the second periodic internal motion (q 2 , b 2 , e 01 , and r 2 ) to zero. Because of the small number of measured transitions for the isotopomers acetone-18 O and -1,3-13 C 2 [3], many parameters transferred from normal acetone had to be kept constant.…”