Effect of isospin on the fusion reaction cross section using various nuclear proximity potentials within the Wong model
Description
Various versions of proximity potentials, with different isospin dependence, are used within the Wong model for fitting the fusion-evaporation cross sections from 58Ni + 58Ni, 64Ni + 64Ni, and 64Ni + 100Mo reactions in an intermediate mass region and capture cross sections from 48Ca + 238U, 244Pu, and 248Cm reactions in a superheavy mass region, known for fusion hindrance phenomena in coupled-channel calculations. It is found that proximity 1988 gives results close to experimental data in a comparison of proximity 1977 and proximity 2000 within the Wong formula, so this Proximity 1988 (Prox 1988) is then used within the extended Wong model. This combination can fit the cross sections for the 58Ni + 58Ni and 64Ni + 64Ni reactions but deviates a little from the experimental data for the 64Ni + 100Mo reaction at a center-of-mass energy below the Coulomb barrier. But the variation of lmax with Ec.m. at sub-barrier energies is absurd for these three reactions. So, a different type of strong nuclear interaction is required that accounts for isospin effect and asymmetry of the colliding nuclei, which is obtained here by a slight adjustment of the coefficient γ0 of the nuclear surface energy constant of the Prox 1988 potential, in order to fit the experimental data for this reaction and named it mod-Prox 1988. The surface energy constant γ depends on the neutron/proton excess, and change in one of its constants, γ0, used in Prox 1988, introduces the required barrier modification for fitting the experimental data. Thus, change in γ leads to change in barrier characteristics, i.e., barrier height (VBl), position (RBl), and oscillator frequency ((ℎ/2π)ωl). Using this modified proximity potential within the extended Wong model, experimental data for all three Ni-induced reactions is fitted with a smooth variation of deduced lmax(Ec.m.) at above- as well as below-barrier energies. The effect of isospin is more prominent at below-barrier energies. As an application, mod-Prox 1988 is then employed for the capture cross-section data from 48Ca + 238U, 244Pu, and 248Cm reactions in superheavy mass regions and it successfully fits the data point to point with a smooth variation of lmax with Ec.m.. Thus, mod-Prox 1988 within the extended Wong model leads to a simultaneous explanation of several reactions displaying a hindrance to fusion. Thus, below the Coulomb barrier a stronger nuclear interaction is required as the N/Z ratio increases and colliding nuclei become more and more asymmetric. The effects of multipole deformations are included here up to hexadecapole in the calculations, and orientation degrees of freedom are integrated for the coplanar configuration.
Additional details
Identifiers
Publishing Information
- Journal Title
- Physical Review. C, Nuclear Physics
- Journal Volume
- 84
- Journal Issue
- 4
- Journal Page Range
- p. 044613-044613.8
- ISSN
- 0556-2813
- CODEN
- PRVCAN
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 43079857
- Subject category
- S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Descriptors DEI
- ASYMMETRY; CALCIUM 48; CAPTURE; COMPARATIVE EVALUATIONS; COULOMB FIELD; COUPLED CHANNEL THEORY; CROSS SECTIONS; CURIUM 248; DEGREES OF FREEDOM; INTERACTIONS; ISOSPIN; MASS; MOLYBDENUM 100; NICKEL 58; NICKEL 64; PLUTONIUM 244; SURFACE ENERGY; URANIUM 238
- Descriptors DEC
- ACTINIDE NUCLEI; ALKALINE EARTH ISOTOPES; ALPHA DECAY RADIOISOTOPES; CALCIUM ISOTOPES; CURIUM ISOTOPES; ELECTRIC FIELDS; ENERGY; EVALUATION; EVEN-EVEN NUCLEI; FREE ENERGY; HEAVY NUCLEI; INTERMEDIATE MASS NUCLEI; ISOTOPES; MOLYBDENUM ISOTOPES; NICKEL ISOTOPES; NUCLEI; PARTICLE PROPERTIES; PHYSICAL PROPERTIES; PLUTONIUM ISOTOPES; RADIOISOTOPES; SPONTANEOUS FISSION RADIOISOTOPES; STABLE ISOTOPES; SURFACE PROPERTIES; THERMODYNAMIC PROPERTIES; URANIUM ISOTOPES; YEARS LIVING RADIOISOTOPES
Optional Information
- Notes
- (c) 2011 American Institute of Physics