Abstract
Very little is known about clustering in heavy nuclei and in particular the interaction between the correlated cluster nucleons and remaining core nucleons. Currently the phenomenological Saxon-Woods plus cubic Saxon-Woods core-cluster potential successfully predicts the alpha decay half-life and energy band spectra of a number of heavy nuclei. This model, however, lacks a microscopic understanding of clustering phenomenon in these heavy nuclear systems. A fully relativistic microscopic formalism is presented, which generates the core-cluster potential by means of the McNeil, Ray and Wallace based double folding procedure. The core and cluster baryon densities are calculated by using a relativistic mean field approach. The Lorentz covariant IA1 representation of the nucleon-nucleon interaction is folded with the core and cluster densities. Theoretical predictions of the ground-state decay half-life and positive parity energy band of 212Po are obtained with the relativistic mean field formalism and which are compared to the results from the phenomenological Saxon-Woods plus cubic Saxon-Wood core-cluster potential and microscopic M3Y interaction. © 2010 IOP Publishing Ltd.
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CITATION STYLE
Wyngaardt, S. M., Groenewald, H. W., Ibrahim, T. T., Ndayishimye, J., & Perez, S. M. (2010). Relativistic mean field formulation of clustering in heavy nuclei. In Journal of Physics: Conference Series (Vol. 205). Institute of Physics Publishing. https://doi.org/10.1088/1742-6596/205/1/012013
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