The Coulombic systems (αpe) and (ααe), (αppe), (ααpe) and (Li 3+ Li 3+ e) placed in a magnetic field B 10 11 G are studied. It is demonstrated a theoretical existence of the exotic ion (He H) 2+ for B 5 × 10 12 G in parallel configuration (the magnetic field is directed along internuclear axis) as optimal as well as its excited states 1π, 1δ. As for the exotic ion He 3+ 2 it is shown that in spite of strong electrostatic repulsion of αparticles this ion can also exist for B 100 a.u. (= 2.35×10 11 G) in parallel configuration as optimal in the states 1σg (ground state), 1πu, 1δg . Upon appearance both ions are unstable towards dissociation with He + in the final state but with very large lifetime. However, at B 10000 a.u., the ion (He H) 2+ becomes stable, while at B 1000 a.u., the ion He 3+ 2 becomes stable. For both ions the vibrational and rotational energies are calculated. With a magnetic field growth, both exotic ions become more and more tightly bound and compact, their lowest rotational and vibrational energies grow drastically. At the edge of applicability of nonrelativistic approximation, B ∼ 4.414 × 10 13 G, there are indications that three more exotic linear ions (H He H) 3+ , (He H He) 4+ and even Li 5+ 2 in parallel configuration may also occur.