This paper reports the assignment of the rotational spectra of the m = 0 and 1 states of 13 CC 5 H 6 -H 2 O and C 6 H 5 D-H 2 O dimers. The m = 1 progression was not identified or assigned for both 13 CC 5 H 6 -H 2 O and C 6 H 5 D-H 2 O in the earlier work, though for the symmetric isotopomers (C 6 H 6 -H 2 O/D 2 O/H 2 18 O), they were identified [H.S. Gutowsky, T. Emilsson, E. Arunan, J. Chem. Phys. 99 (1993) 4883]. The m = 1 transitions for 13 CC 5 H 6 -H 2 O and C 6 H 5 D-H 2 O were split into two, unlike that of the parent C 6 H 6 -H 2 O isotopomer. The splitting varied, somewhat randomly, with quantum numbers J and K. The m = 0 lines of 13 CC 5 H 6 -H 2 O had significant overlap with the m = 1 lines of the parent isotopomer, clouding proper assignment, and leading to an rms deviation of about 200 kHz in the earlier work. The general semi-rigid molecular Hamiltonian coupled to an internal rotor, described recently by Duan et al. [Y.B. Duan, H.M. Zhang, K. Takagi, J. Chem. Phys. 104 (1996) 3914], is used in this work to assign both m = 0 and 1 states of 13 CC 5 H 6 -H 2 O and C 6 H 5 D-H 2 O dimers. Consequently, the m = 0 fits for 13 CC 5 H 6 -H 2 O/D 2 O have an rms deviation of only 4/ 7 kHz, comparable to experimental uncertainties. The fits for m = 1 transitions for 13 CC 5 H 6 -H 2 O and C 6 H 5 D-H 2 O dimers have an rms deviation of about 200 kHz.However, it is of the same order of magnitude as that of the m = 1 state of the parent C 6 H 6 -H 2 O dimer. The A rotational constants determined from the m = 0 fits for both 13 CC 5 H 6 -H 2 O and 13 CC 5 H 6 -D 2 O isotopomers are identical and very close to the C rotational constant for 13 CC 5 H 6 . This provides a direct experimental determination for the C rotational constant of 13 CC 5 H 6 , which has a negligible dipole moment.