Complexes of chlorobenzene and ammonia, C6H5ChNH3, C,&Cl(NH3)2, and C&I5Cl(NH3)3, were studied by single-photon ionization. The ionization potentials of these three complexes were measured to be 8.744 f 0.022, 8.652 f 0.013, and 8.555 f 0.012 eV, respectively. The appearance potential of C6HsNH3+ from C6H5CbNH3 was found at 8.935 f 0.004 eV, which, with the known heat of formation of anilinium ion, gives the dissociation energy D(c6H~cbNH3) = 2.9 f 0.5 kcal mol-' (12.0 f 2.2 kJ mol-'). Then, from its onset energy from C6H5ChNH3, the dissociation energy of ( C~H S C~. N H~) + is calculated to be D[(C6H&l.NH3)+] = 10.4 f 0.7 kcal mol-' (43.5 f 2.9 kJ mol-'), unusually large for a heterodimer ion. No production of C&NH3+ from trimers could be detected in the onset region. The ion C&NH2+ has onsets of 8.849 f 0.009 and 8.855 f 0.029 eV from C6HsCbNH3 and C6H&l(NH3)2, respectively. These energies are below the onset for C6H5NH3+ but far above the thermochemical thresholds for aniline ion, which are near 7.6 eV. Evidently, C6HsNH2+ is not produced by dissociative ionization of the excited neutral complex. Instead, the complex must first be ionized and excited to at least 0.1 eV. Since the onsets for (C~HSCI*NH~)+ and C&NH2+ are lower than for C&NH3+, then (C&Cl-NH3)+ in its ground state does not spontaneously form CaH5NH3+. Kinetic energy release distributions measured for C&NH2+ and CaH5NH3+ indicate that the formation of both ions is consistent with statistical processes; i.e., no evidence for nonstatistical mechanisms was found, even for photon energies as large as 17.7 eV.