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In our previous publications we discussed various manifestations of a newdecay channel of the low excited heavy nuclei called collinear clustertri-partition (CCT). The most populated CCT mode was revealed in the masscorrelation distribution of fission fragments (FFs) as a local region ("bump")of increased yields below the loci linked to the conventional binary fission.The bump was dubbed "Ni-bump" because it is centered at the masses associatedwith the magic isotopes of Ni. Intriguing features of the CCT, especially highcollinearity of the CCT partners and relatively high probability comparablewith that typical for conventional ternary fission, have caused rather widediscussion. In the majority of dedicated publications, the FFs partitions fromthe Ni-bump have been analyzed from the different points of view. In ourpublications, we have underlined that Ni-bump manifests itself at thedetectable level only in the spectrometer arm that faces the source backing. Sofar, this fact has been left beyond the scope of all known theoreticalconsiderations, while the backing likely plays a crucial role in theobservation of the CCT experimental pattern.

Refined scenario of the collinear cluster tri-partition mode with the greatest yield