Abstract. With the observation of the collinear cluster tripartition in 252 Cf, we discuss various features of the true ternary fission (collinear fission). The conditions for collinear ternary decay with three clusters are explained. We discuss the potential energy surfaces for ternary decay and conditions for the collinear decay.
Collinear ternary fissionTernary fission with comparable masses is a process which occurs in heavy nuclei under conditions of large values of Z 2 /A, called the fission-parameter. The decay into three fragments (true ternary fission) observed is found to be collinear. Recent experiments for the spontaneous decay of 252 Cf(fff) and of neutron induced fission in 235 U(n,fff), using the missing mass approach with two FOBOS-detectors in coincidence at 180 o , see ref. [1,2], true ternary fission has been observed with the missing mass method. In this new kind of radioactive fission decay, the so called collinear cluster tripartition (CCT), the three fragments are emitted collinear, here typical fragments are isotopes of Sn, Ni, and Ca. The latter, Ca, as the third particle is positioned along the line connecting Sn and Ni. This exotic decay can be understood as a breakup of very elongated (hyper-deformed) shapes with two neck ruptures.From three different experiments reported in ref.[1, 2] on CCT, an overall yield of 4× 10 −3 /(binary fission) has been observed. This result has been considered to have unusually high values, when compared with the previously known yields in "ternary fission" with the emission of lighter fragments perpendicular to the fission axis [3,4].This high probability can be explained if the phase space for the CCT-decay is considered (see also [5,6]). The phase space depends on, i)the potential energy surfaces (PES), ii) the Q-values, the latter determining the number of possible isotope combinations, iii) the excitation energy range in the individual fragments, iv) the momentum range, v) the number of excited states (density of states) in combinations consisting of 2(3) isotopes, vi) the number of excited states in each fragment, and vii) the spin (J) multiplicity in these states with spins up to (6-8) + (phase space factor (2J+1)). Fragments with odd numbers of protons and/or neutrons have in addition a particular large density of states.The question of the relative importance of fission through oblate or prolate shapes (chain configurations) has been addressed repeatedly [7][8][9]. Within the three cluster model, it has been shown, that the collinear configuration is the favoured mode over the oblate configuration [9] for the ternary a