1987
DOI: 10.1103/physrevlett.59.2856
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Asymmetric Fission ofNi56

Abstract: Cross sections for the two-body channels populated in the 32 S+ 24 Mg reaction at E c . m . =60.8 MeV have been measured by use of a coincidence technique which allows correction for secondary lightparticle evaporation. The data show reaction yields with full equilibration of energy and massasymmetry coordinates. These results suggest an asymmetric fission mechanism and are contrary to what is expected from the previously proposed "orbiting" mechanism in light systems.

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Cited by 64 publications
(58 citation statements)
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“…Note that 56 N i is a negative Q-value system (negative Q out , different for different exit channels) and hence would decay only if it were produced in heavy ion reactions with sufficient compound nucleus excitation energy E * CN (= E cm + Q in ), to compensate for the negative Q out , the deformation energy of fragments E d , their total kinetic energy TKE and the total excitation energy TXE, in the exit channel, as to the hot 56 N i * nucleus data from Refs. [2,3] in section 3. The (statistical) evaporation of light particles, that occur promptly before the beginning of the binary decay process of cluster emission studied here, is not included in this paper.…”
Section: Experimentallymentioning
confidence: 99%
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“…Note that 56 N i is a negative Q-value system (negative Q out , different for different exit channels) and hence would decay only if it were produced in heavy ion reactions with sufficient compound nucleus excitation energy E * CN (= E cm + Q in ), to compensate for the negative Q out , the deformation energy of fragments E d , their total kinetic energy TKE and the total excitation energy TXE, in the exit channel, as to the hot 56 N i * nucleus data from Refs. [2,3] in section 3. The (statistical) evaporation of light particles, that occur promptly before the beginning of the binary decay process of cluster emission studied here, is not included in this paper.…”
Section: Experimentallymentioning
confidence: 99%
“…For the 32 S + 24 M g → 56 N i * reaction, in one of the experiments, the mass spectra for A=12 to 28 fragments and the total kinetic energy (TKE) for only the most favoured (enhanced yields) α-nucleus fragments are measured at the energies E lab = 121.1 and 141.8 MeV, or equivalently at E cm =51.6 and 60.5 MeV, respectively [2,3]. Note that 56 N i is a negative Q-value system (negative Q out , different for different exit channels) and hence would decay only if it were produced in heavy ion reactions with sufficient compound nucleus excitation energy E * CN (= E cm + Q in ), to compensate for the negative Q out , the deformation energy of fragments E d , their total kinetic energy TKE and the total excitation energy TXE, in the exit channel, as to the hot 56 N i * nucleus data from Refs.…”
Section: Experimentallymentioning
confidence: 99%
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“…On the other hand reactions which produce three or more heavy fragments are known to be strongly suppressed in this energy regime. During the last two decades, considerable effort has been devoted to the understanding of the binary-reaction processes in heavy-ion collisions within the framework of a systematic study of the fusion-fission process (FF) for light-mass (20 ≤ A CN ≤ 60) composite systems [1][2][3][4][5][6][7][8][9][10][11][12][13]. It has been shown for example that entrance-channel effects do not play a significant role in the binary-decay processes of the 47 [7]) at comparable excitation energies and angular momenta.…”
Section: Introductionmentioning
confidence: 99%