The process of recombination of a bare heavy nucleus with an electron via the creation of a free-poistron-bound-electron pair was discussed. The process was denoted as 'negative-continuum dielectronic recombination' as it resulted in the capture of an incident electron into a bound state accompanied by a transition of a negative-continuum electron into a bound state. For a wide range of incident electron energies for Z = 82 and 92, the calculations were performed.