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Production of neutron-enriched isotopes along magic number N = 126 by multinucleon transfer reactions with radioactive-ion beams
被引:0
|作者:
Saiko, V. V.
[1
,2
,3
]
V. Karpov, A.
[1
,3
]
机构:
[1] JINR, Flerov Lab Nucl React, Dubna 141980, Russia
[2] Inst Nucl Phys, Alma Ata 050032, Kazakhstan
[3] Dubna State Univ, Dubna 141982, Russia
关键词:
LANGEVIN DESCRIPTION;
N/Z-EQUILIBRATION;
RICH ISOTOPES;
FISSION;
FUSION;
COLLISIONS;
NUCLIDES;
DYNAMICS;
D O I:
10.1103/PhysRevC.109.064607
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: Multinucleon transfer (MNT) processes in low -energy deep inelastic (damped) collisions of heavy ions can be employed to produce heavy neutron -enriched nuclei. Recent progress in development of radioactiveion beam (RIB) facilities may give additional possibilities in producing nuclei with large neutron excess. Purpose: A major aim of the work is to calculate the cross sections of heavy neutron -rich isotopes with the magic number N = 126 in the reactions 132 Sn + 198 Pt and 136 , 138 , 140 Xe + 198 Pt within a multidimensional dynamical model based on the Langevin equations. Another purpose of the paper is to study the relative production rates of such nuclei reachable at currently working RIB facilities. Method: A multidimensional dynamical model of nucleus -nucleus collisions based on the Langevin equations [A. V. Karpov and V. V. Saiko, Phys. Rev. C 96 , 024618 (2017)] has been used in the present work. This model provides a reasonable description of available experimental data. Results: Cross sections of heavy neutron -enriched nuclides obtained in the MNT reactions 132 Sn + 198 Pt and 136 , 138 , 140 Xe + 198 Pt have been calculated. Relative production rates of these nuclei were estimated using beam intensities available at currently working RIB facilities. Conclusions: Using neutron -rich radioactive projectiles in multinucleon transfer reactions with the 198 Pt target, one can reach an order of magnitude higher cross sections of neutron -enriched nuclides with the magic number N = 126. Relative production yields of such nuclei increase with the increasing N / Z ratio of the projectile.
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