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Title: Extension of the nuclear landscape to hyperheavy nuclei

Abstract

The properties of hyperheavy nuclei and the extension of nuclear landscape to hyperheavy nuclei are extensively studied within covariant density functional theory. Axial reflection symmetric and reflection asymmetric relativistic Hartree-Bogoliubov (RHB) calculations are carried out. The role of triaxiality is studied within triaxial RHB and triaxial relativistic mean field + BCS frameworks. With increasing proton number beyond Z 130 the transition from ellipsoidal-like nuclear shapes to toroidal ones takes place. The description of latter shapes requires the basis which is typically significantly larger than the one employed for the description of ellipsoidal-like shapes. Many hyperheavy nuclei with toroidal shapes are expected to be unstable toward multifragmentation. Yet, three islands of stability of spherical hyperheavy nuclei have been predicted for the first time in Afanasjev et al. [Phys. Lett. B 782, 533 (2018)]. Proton and neutron densities, charge radii, neutron skins, and underlying shell structure of the nuclei located in the centers of these islands have been investigated in detail. Large neutron shell gaps at N = 228 , 308 , and 406 define approximate centers of these islands in neutron number. On the contrary, large proton gap appear only at Z = 154 in the ( Z 156 , N 310 ) island. As a result, this is the largest island of stability of spherical hyperheavy nuclei found in the calculations. The calculations indicate the stability of the nuclei in these islands with respect to octupole and triaxial distortions. The shape evolution of toroidal shapes along the fission path and the stability of such shapes with respect to fission have been reported on. Fission barriers in neutron-rich superheavy nuclei are studied in triaxial RHB framework; the impact of triaxiality on the heights of fission barriers is substantial in some parts of this region. Based on the results obtained in the present work, the extension of nuclear landscape to hyperheavy nuclei is provided.

Authors:
 [1];  [2];  [1];  [1]
  1. Mississippi State Univ., Mississippi State, MS (United States)
  2. Mississippi State Univ., Mississippi State, MS (United States); Kyoto Univ. (Japan)
Publication Date:
Research Org.:
Mississippi State Univ., Mississippi State, MS (United States)
Sponsoring Org.:
USDOE National Nuclear Security Administration (NNSA); USDOE Office of Science (SC), Nuclear Physics (NP)
OSTI Identifier:
1597108
Alternate Identifier(s):
OSTI ID: 1500135
Grant/Contract Number:  
SC0013037; NA0002925
Resource Type:
Accepted Manuscript
Journal Name:
Physical Review C
Additional Journal Information:
Journal Volume: 99; Journal Issue: 3; Journal ID: ISSN 2469-9985
Publisher:
American Physical Society (APS)
Country of Publication:
United States
Language:
English
Subject:
73 NUCLEAR PHYSICS AND RADIATION PHYSICS

Citation Formats

Agbemava, S. E., Afanasjev, Anatoli V., Taninah, A., and Gyawali, A. Extension of the nuclear landscape to hyperheavy nuclei. United States: N. p., 2019. Web. doi:10.1103/PhysRevC.99.034316.
Agbemava, S. E., Afanasjev, Anatoli V., Taninah, A., & Gyawali, A. Extension of the nuclear landscape to hyperheavy nuclei. United States. https://doi.org/10.1103/PhysRevC.99.034316
Agbemava, S. E., Afanasjev, Anatoli V., Taninah, A., and Gyawali, A. Fri . "Extension of the nuclear landscape to hyperheavy nuclei". United States. https://doi.org/10.1103/PhysRevC.99.034316. https://www.osti.gov/servlets/purl/1597108.
@article{osti_1597108,
title = {Extension of the nuclear landscape to hyperheavy nuclei},
author = {Agbemava, S. E. and Afanasjev, Anatoli V. and Taninah, A. and Gyawali, A.},
abstractNote = {The properties of hyperheavy nuclei and the extension of nuclear landscape to hyperheavy nuclei are extensively studied within covariant density functional theory. Axial reflection symmetric and reflection asymmetric relativistic Hartree-Bogoliubov (RHB) calculations are carried out. The role of triaxiality is studied within triaxial RHB and triaxial relativistic mean field + BCS frameworks. With increasing proton number beyond Z≈130 the transition from ellipsoidal-like nuclear shapes to toroidal ones takes place. The description of latter shapes requires the basis which is typically significantly larger than the one employed for the description of ellipsoidal-like shapes. Many hyperheavy nuclei with toroidal shapes are expected to be unstable toward multifragmentation. Yet, three islands of stability of spherical hyperheavy nuclei have been predicted for the first time in Afanasjev et al. [Phys. Lett. B 782, 533 (2018)]. Proton and neutron densities, charge radii, neutron skins, and underlying shell structure of the nuclei located in the centers of these islands have been investigated in detail. Large neutron shell gaps at N=228,308, and 406 define approximate centers of these islands in neutron number. On the contrary, large proton gap appear only at Z=154 in the (Z≈156,N≈310) island. As a result, this is the largest island of stability of spherical hyperheavy nuclei found in the calculations. The calculations indicate the stability of the nuclei in these islands with respect to octupole and triaxial distortions. The shape evolution of toroidal shapes along the fission path and the stability of such shapes with respect to fission have been reported on. Fission barriers in neutron-rich superheavy nuclei are studied in triaxial RHB framework; the impact of triaxiality on the heights of fission barriers is substantial in some parts of this region. Based on the results obtained in the present work, the extension of nuclear landscape to hyperheavy nuclei is provided.},
doi = {10.1103/PhysRevC.99.034316},
journal = {Physical Review C},
number = 3,
volume = 99,
place = {United States},
year = {Fri Mar 15 00:00:00 EDT 2019},
month = {Fri Mar 15 00:00:00 EDT 2019}
}

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Cited by: 17 works
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