Abstract:Emission of ~He in the reaction 334MeV 4~ has been studied by triple coincidence measurements that allow the separate identification of fusion fission and sequential fission. For the 4He evaporative spectra from fusion fission the composite system is shown to be the predominant contributor; whereas, for sequential fission the dominant emission is from the fragments. This result demonstrates a correlation between evaporative emission probability and lifetime expectancy of the composite system. To account for th… Show more
“…This fact, together with the results of [12,13] implies that the probability of ternary fission increases with the excitation energy of the fissioning system.…”
Section: =~mentioning
confidence: 57%
“…The geometrical factors were taken from the reaction simulation, as it was done in [12]. The multiplicities calculated for the 12C+197Au system are: McN E=0.025_+0.006 for alpha evaporation from the compound nucleus and MFFE=0.008 0.003 for the fragment emission.…”
Section: Alpha Multiplicities For the Cne Ffe And Tfe Processesmentioning
The results of coincidence measurements of 4He emission with fission fragments in reactions of 12C(108 MeV) ions with a 19VAu target and of 160(144MeV) ions with a 232Th target are presented. On the basis of a Monte Carlo kinematic simulation of nuclear reactions the experimental energy spectra and velocity distributions of alpha particles have been analyzed. A conclusion has been drawn that the main source of 4He emission is evaporation from the fissioning compound nucleus. Substantial part of alpha particles was emitted from fully accelerated fission fragments. Some of 4He nuclei with an average energy of about 16 MeV (in the CM system) emitted mainly perpendicular to the fission axis were identified as being similar long-range alpha particles produced in ternary fission of heavy nuclei at a low excitation energy. The emission multiplicities of these particles are considerably higher than those observed at a low excitation energy. The experimental results are compared with the statistical model predictions. 24.60.Dr
PACS"
“…This fact, together with the results of [12,13] implies that the probability of ternary fission increases with the excitation energy of the fissioning system.…”
Section: =~mentioning
confidence: 57%
“…The geometrical factors were taken from the reaction simulation, as it was done in [12]. The multiplicities calculated for the 12C+197Au system are: McN E=0.025_+0.006 for alpha evaporation from the compound nucleus and MFFE=0.008 0.003 for the fragment emission.…”
Section: Alpha Multiplicities For the Cne Ffe And Tfe Processesmentioning
The results of coincidence measurements of 4He emission with fission fragments in reactions of 12C(108 MeV) ions with a 19VAu target and of 160(144MeV) ions with a 232Th target are presented. On the basis of a Monte Carlo kinematic simulation of nuclear reactions the experimental energy spectra and velocity distributions of alpha particles have been analyzed. A conclusion has been drawn that the main source of 4He emission is evaporation from the fissioning compound nucleus. Substantial part of alpha particles was emitted from fully accelerated fission fragments. Some of 4He nuclei with an average energy of about 16 MeV (in the CM system) emitted mainly perpendicular to the fission axis were identified as being similar long-range alpha particles produced in ternary fission of heavy nuclei at a low excitation energy. The emission multiplicities of these particles are considerably higher than those observed at a low excitation energy. The experimental results are compared with the statistical model predictions. 24.60.Dr
PACS"
“…From the energetic position of both, the deficit and surplus anomaly and the obvious correlation with the scission axis we infer that both are related and have to be attributed to a near-scission emission process. A surplus anomaly has also been observed in the c~ emission of 8.4 MeV/n 4~ [4] and 10 MeV/n 35Cl+natAg [-5] and was interpreted as near-scission emission.…”
Section: A Inplane Correlation Datamentioning
confidence: 92%
“…From previous experiments [- 1,3,4,5,19] it is known that the spectra are dominated by sequential light particle emission from composite nucleus (CNE) and from fully accelerated fission fragments (FE). In a standard 3-source calculation [5,20,21] the reaction kinematics were defined by the measured velocity distribution of the fragments; the energy distribution of the primary fragments was parametrized by a Gaussian distribution, the mean and standard deviation of which were taken from the measured distributions.…”
Section: Sources Of Sequential Light-particle Emissionmentioning
“…In this paper we report the results of such multiplicity determinations for composite-nucleus evaporation (CE) and fragment evaporation (FE). We examine the behaviour of four reaction systems each with incident laboratory energy of 8.5 MeV/u: 4~ +"atAg [26], 56Fe+natAg [27], 4~ [28], 56Fe -~-238U [29], Our main purpose is to compare the multiplicities for evaporative processes and to preview the kind of information that can be obtained from such investigations. We will only outline the kinematic analysis and defer the details to forthcoming papers [26][27][28][29].…”
Multiplicities are compared for 4He evaporation in reactions of 4~ and 56Fe projectiles (8.5 MeV/u) with with "atAg and 238U targets. Coincidence requirements involving fusion-fission and projectile-like fragments have been used to select separate entrance-channel spin zones. Evaporation-like 4He emission from the composite nuclei is shown to be large for mean spins < 100h, and to decrease dramatically with increasing spin. Coincidence measurements between two 4He particles have also been studied for *~ This requirement is shown to select reactions that lead to evaporation residues and therefore to a zone of relatively low spin. The shapes of the 4He spectra provide an interesting probe of the mechanism and also of the thermodynamic properties of hot nuclei.
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