Bulletin of the American Physical Society
2021 Fall Meeting of the APS Division of Nuclear Physics
Volume 66, Number 8
Monday–Thursday, October 11–14, 2021; Virtual; Eastern Daylight Time
Session LM: Nuclear Theory VI
2:00 PM–3:48 PM,
Wednesday, October 13, 2021
Room: White Hill
Chair: Charlotte Elster, Ohio University
Abstract: LM.00007 : Extending the limits of nuclear landscape via new physical mechanisms*
3:12 PM–3:24 PM
Presenter:
Anatoli Afanasjev
(Mississippi State University)
Authors:
Anatoli Afanasjev
(Mississippi State University)
Sylvester E Agbemava
(National Superconducting Cyclotron Labor)
Ahmad Taninah
(Mississippi State Univ)
saja A Teeti
(Mississippi State Univ)
the nuclear landscape beyond the traditional limits has been performed over recent years. In the region
of hyperheavy (Z>126) nuclei, the transition from ellipsoid-like nuclear shapes to toroidal ones
provides a substantial increase of nuclear landscape [1-3]. Rotational excitations in the nuclei
near proton and neutron drip lines provide an alternative mechanism for an extension of the nuclear
landscape beyond the limits defined at spin zero [4,5]. In both cases, the collective coordinates related
to nuclear shapes play an important role in extending nuclear landscape. In hyperheavy nuclei, they
drive the nuclear systems from ellipsoidal-like to toroidal shapes. In rotating nuclei, triggered by
particle-hole excitations they transform the system from spherical or normal deformed ground
states to extremely elongated (super-, hyper and mega-deformed) shapes or rotation-induced
proton halos at high spins. Rotational frequency acts as an additional collective degree of freedom
(coordinate) in rotating nuclei. At the microscopic level, the impact of these collective coordinates drives
the single-particle orbitals, which are otherwise located at positive energy in a given nucleonic
configuration, below the continuum threshold. As a consequence, it allows to extend the limits of nuclear
landscape beyond traditional limits (for example, beyond spin-zero drip lines in rotating nuclei). The
similarities and differences of these mechanisms will be discussed. The roles of underlying single-particle
and shell structures will be analyzed.
*This material is based upon work supported by theU.S. Department of Energy, Office of Science, Office ofNuclear Physics under Award No. DE-SC0013037
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