has been investigated by theoretical calculations at MP2 and CCSD(T) levels with large basis sets. Transition structures (TSs) for the loss of an H atom and formation of the FHF Ϫ and ClHCl Ϫ anions were located by analytic methods. Initial electron attachment to HF.HF dimer occurs without activation and yields a dipole-bound anion state (DBS) as shown previously. Reaction (1) is endothermic by 65.8 kJ/mol at the CCSD(T)/augcc-pVDZ level. An intermediate ion-induced dipole complex between H ⅐ and FHF Ϫ is reached from the DBS over a potential barrier of 66.6 kJ/mol. Analysis of the charge distribution as a function of the distance to the departing H ⅐ reveals that the diffuse DBS collapses to a much more compact valence configuration prior to the TS being reached. In the valence configuration, the electron occupies the * orbital of the terminal HOF bond. DA to HCl.HCl differs from the fluorine case in several important respects. HCl.HCl does not form a DBS. Rather, electron attachment occurs by direct insertion into the * orbital of the terminal HOCl bond with an activation energy of 20.3 kJ/mol. As in the fluorine case, electron capture occurs before the TS. The electron density collapses to a valence configuration when the HOCl bond is stretched to about 1.45 Å, intermediate between that in the neutral dimer, 1.28 Å, and in the TS to DA, 1.57 Å. A "T-shaped" ion-induced dipole complex, bound by about 2 kJ/mol, lies between the TS and the separated H atom and ClHCl Ϫ anion products. With respect to DA, the chlorine system is intermediate between the fluorine system and the previously reported bromine system. The latter was found to undergo DA with a 0.0-kJ/mol barrier.