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Phys. Rev. C 33, 143–152 (1986)

Preequilibrium neutron emission in fusion of 165Ho+12C at 25 MeV per nucleon

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E. Holub, D. Hilscher, G. Ingold, U. Jahnke, H. Orf, H. Rossner, and W. P. Zank
Hahn-Meitner-Institut für Kernforschung Berlin, 1000 Berlin 39, Federal Republic of Germany

W. U. Schröder
Department of Chemistry and Nuclear Structure Research Laboratory, University of Rochester, Rochester, New York 14627

H. Gemmeke
Fachbereich Physik der Philipps Universitat Marburg, 3550 Marburg, Federal Republic of Germany

K. Keller, L. Lassen, and W. Lücking
Physikalisches Institut der Universitat Heidelberg, 6900 Heidelberg, Federal Republic of Germany

Received 1 August 1985; published in the issue dated January 1986

Neutrons were measured in coincidence with evaporation residues from the reaction 165Ho+(300 MeV) 12C. The evaporation residue velocity distribution is indicative of an average transfer of 80% of the full linear momentum in this reaction. The energy spectra of the coincident neutrons exhibit evaporative and preequilibrium components associated with integral multiplicities of MEV=(9.5±0.5) and MPE=(1.7±0.3), respectively. The experimental neutron energy and angular distributions are analyzed in terms of multiple-source parametrizations, assuming two or three emitters. The results are compared to those obtained from other inclusive and exclusive associated-particle data. It is observed that the emission patterns of the preequilibrium neutrons are in accord with the predictions of a Fermi-jet model, for neutron angles forward of 35°, while this model fails to reproduce the data at angles in the vicinity of 90° and beyond. Various different nucleon momentum distributions have been employed in the model comparison. The insufficiency of the Fermi-jet model to reproduce the data is attributed to the neglect of two-body collisions in this one-body theory. In contrast, the shape of the angle-integrated preequilibrium-neutron energy spectrum is well reproduced with the Harp-Miller-Berne preequilibrium model, if an initial exciton number of n0=15 is adopted. This value, as well as the preequilibrium neutron multiplicity, is at variance with systematics established previously.

© 1986 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.33.143
DOI:
10.1103/PhysRevC.33.143
PACS:
25.70.Gh, 25.70.Jj