Detailed statistical model analysis of observables from fusion-fission reactions

被引:18
|
作者
Banerjee, Tathagata [1 ,2 ]
Nath, S. [1 ]
Pal, Santanu [1 ,3 ]
机构
[1] Inter Univ Accelerator Ctr, Nucl Phys Grp, Aruna Asaf Ali Marg,Post Box 10502, New Delhi 110067, India
[2] Australian Natl Univ, Res Sch Phys & Engn, Dept Nucl Phys, Canberra, ACT 0200, Australia
[3] Variable Energy Cyclotron Ctr, Phys Grp, 1-AF Bidhan Nagar, Kolkata 700064, India
关键词
ALPHA-PARTICLE EMISSION; PROTON-INDUCED FISSION; ANGULAR-MOMENTUM; NEUTRON EMISSION; TIME SCALES; PROMPT NEUTRONS; LEVEL DENSITY; HIGH-SPIN; PREEQUILIBRIUM EMISSION; COLLECTIVE ENHANCEMENT;
D O I
10.1103/PhysRevC.99.024610
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
Background: Despite remarkable success of the statistical model (SM) in describing decay of excited compound nuclei (CN), reproduction of the observables from heavy ion-induced fusion-fission reactions is often quite challenging. Ambiguities in choosing the input parameters, lack of clarity about inclusion of various physical effects in the model, and contradictory requirements of input parameters while describing different observables from similar reactions are among the major difficulties of modeling decay of fissile CN. Purpose: This work attempts to overcome the existing inconsistencies by inclusion of important physical effects in the model and through a systematic analysis of a large set of data over a wide range of CN mass (A(CN)). Method: The model includes the shell effect in the level density (LD) parameter, shell correction in the fission barrier (B-f), the effect of the orientation degree of freedom of the CN spin (K-or), collective enhancement of level density (CELD), and dissipation in fission. Input parameters are not tuned to reproduce observables from specific reaction(s) and the reduced dissipation coefficient (beta) is treated as the only adjustable parameter. Calculated evaporation residue (ER) cross sections (sigma(ER)), fission cross sections (sigma(fiss)), and particle, i.e., neutron, proton, and alpha particle, multiplicities are compared with data covering A(CN) = 156-248. Results: The model produces reasonable fits to ER and fission excitation functions for all the reactions considered in this work. Pre-scission neutron multiplicities (nu(pre)) are underestimated by the calculation beyond A(CN) similar to 200. An increasingly higher value of beta, in the range of 2-4 x 10(21) s(-1), is required to reproduce the data with increasing A(CN). Proton and alpha-particle multiplicities, measured in coincidence with both ERs and fission fragments, are in qualitative agreement with model predictions. Conclusions: The present work mitigates the existing inconsistencies in modeling statistical decay of the fissile CN to a large extent. Contradictory requirements of fission enhancement-obtained by scaling down the fission barrier to reproduce sigma(ER) or sigma(fiss) and fission suppression realized by introducing dissipation in the fission channel to reproduce nu(pre), for similar reactions-have now become redundant. There are scopes for further refinement of the model, as is evident from the mismatch between measured and calculated particle multiplicities in a few cases.
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页数:13
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