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We consider a possibility of capture of a heavy charged massive particle$\chi^-$ by the nucleus leading to appearance of a bound state. A simpleanalytic formula allowing to calculate binding energies of the $N\chi^-$ boundstate for different nuclei is derived. If the binding energy is sufficientlylarge the particle $\chi^-$ is stable inside the nucleus. The probabilities ofthe nuclear fissions for such states are calculated. It is shown that the boundstates are more stable to a possible fission in comparison to the bare nucleus.This makes an observation of this hypothetical charged massive particle and thesuperheavy nuclei more probable.

Binding energy and fission of the heavy charged massive particle - nucleus bound state