2013/09/12 by A. V. Afanasjev, S. E. Agbemava, S. E. Abgemava +2 · 2 citations
Materials Science · Physics and Astronomy · #Astronomical and nuclear sciences #Atomic physics #Covariant transformation #Geometry #Line (geometry) #Neutron #Nuclear drip line #Nuclear physics #Nuclear physics research studies #Open shell #Physics #Proton #Quantum mechanics #Shell (structure) #X-ray Diffraction in Crystallography #nucl-th
paper · pdf · doi:10.1016/j.physletb.2013.09.017
published as Physics Letter B 726, 680 (2013) · 6 pages, 4 figures, Physics Letters B, in press
arxiv created 2013/09/12 · openalex publication_date 2013/09/17 · arxiv updated 2015/06/17 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The neutron and proton drip lines represent the limits of the nuclear landscape. While the proton drip line is measured experimentally up to rather high Z-values, the location of the neutron drip line for absolute majority of elements is based on theoretical predictions which involve extreme extrapolations. The first ever systematic investigation of the location of the proton and neutron drip lines in the covariant density functional theory has been performed by employing a set of the state-of-the-art parametrizations. Calculated theoretical uncertainties in the position of two-neutron drip line are compared with those obtained in non-relativistic DFT calculations. Shell effects drastically affect the shape of two-neutron drip line. In particular, model uncertainties in the definition of two-neutron drip line at Z∼ 54, N=126 and Z∼ 82, N=184 are very small due to the impact of spherical shell closures at N=126 and 184.