The weakly bound diatomic systems 4 He 2 and 4 HeH Ϫ have been found able to support only one bound state for Jϭ0, although the latter also supports an additional bound state for Jϭ1. In the present paper we, therefore, study the structure of the bound states which might exist for the weakly bound triatomic 4 He 2 H Ϫ , in its Jϭ0 state, by describing the full potential as a simple addition of two-body ͑2B͒ interactions. We carry out bound state calculations using both Jacobi coordinates within a discrete variable representation ͑DVR͒ and pair coordinates with a distributed Gaussian function ͑DGF͒ expansion. The system is shown to possess two bound states with respect to its lower dissociation threshold and two further ''ghost'' states before the complete break-up threshold. The spatial structures of such states and of the floppy complex are analyzed in detail, as is the possibility of detecting Efimov-type states in such a weakly bound aggregate. Finally, the inclusion of three-body ͑3B͒ forces in the description of the full interaction and its effect on the number of possible bound states is also discussed.