Nuclear ground-state masses and deformations: FRDM(2012)
Abstract
Here, we tabulate the atomic mass excesses and binding energies, ground-state shell-plus-pairing corrections, ground-state microscopic corrections, and nuclear ground-state deformations of 9318 nuclei ranging from 16O to A=339. The calculations are based on the finite-range droplet macroscopic and the folded-Yukawa single-particle microscopic nuclear-structure models, which are completely specified. Relative to our FRDM(1992) mass table in Möller et al. (1995), the results are obtained in the same model, but with considerably improved treatment of deformation and fewer of the approximations that were necessary earlier, due to limitations in computer power. The more accurate execution of the model and the more extensive and more accurate experimental mass data base now available allow us to determine one additional macroscopic-model parameter, the density-symmetry coefficient LL, which was not varied in the previous calculation, but set to zero. Because we now realize that the FRDM is inaccurate for some highly deformed shapes occurring in fission, because some effects are derived in terms of perturbations around a sphere, we only adjust its macroscopic parameters to ground-state masses.
- Authors:
-
- Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
- Kyoto Univ., Kyoto (Japan)
- RIKEN Nishina Center, Wako (Japan); Center for Mathematics and Physics Univ. of Aizu, Fukushima (Japan)
- Publication Date:
- Research Org.:
- Los Alamos National Laboratory (LANL), Los Alamos, NM (United States)
- Sponsoring Org.:
- USDOE National Nuclear Security Administration (NNSA)
- OSTI Identifier:
- 1248866
- Alternate Identifier(s):
- OSTI ID: 1325396
- Report Number(s):
- LA-UR-15-26310
Journal ID: ISSN 0092-640X; PII: S0092640X1600005X
- Grant/Contract Number:
- FG02-06ER41407; 25287065; AC52-06NA25396
- Resource Type:
- Journal Article: Accepted Manuscript
- Journal Name:
- Atomic Data and Nuclear Data Tables
- Additional Journal Information:
- Journal Volume: 109-110; Journal Issue: C; Journal ID: ISSN 0092-640X
- Publisher:
- Elsevier
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 73 NUCLEAR PHYSICS AND RADIATION PHYSICS; nuclear masses; fission-barrier heights; ground-state deformations
Citation Formats
Moller, P., Sierk, A. J., Ichikawa, T., and Sagawa, H. Nuclear ground-state masses and deformations: FRDM(2012). United States: N. p., 2016.
Web. doi:10.1016/j.adt.2015.10.002.
Moller, P., Sierk, A. J., Ichikawa, T., & Sagawa, H. Nuclear ground-state masses and deformations: FRDM(2012). United States. https://doi.org/10.1016/j.adt.2015.10.002
Moller, P., Sierk, A. J., Ichikawa, T., and Sagawa, H. 2016.
"Nuclear ground-state masses and deformations: FRDM(2012)". United States. https://doi.org/10.1016/j.adt.2015.10.002. https://www.osti.gov/servlets/purl/1248866.
@article{osti_1248866,
title = {Nuclear ground-state masses and deformations: FRDM(2012)},
author = {Moller, P. and Sierk, A. J. and Ichikawa, T. and Sagawa, H.},
abstractNote = {Here, we tabulate the atomic mass excesses and binding energies, ground-state shell-plus-pairing corrections, ground-state microscopic corrections, and nuclear ground-state deformations of 9318 nuclei ranging from 16O to A=339. The calculations are based on the finite-range droplet macroscopic and the folded-Yukawa single-particle microscopic nuclear-structure models, which are completely specified. Relative to our FRDM(1992) mass table in Möller et al. (1995), the results are obtained in the same model, but with considerably improved treatment of deformation and fewer of the approximations that were necessary earlier, due to limitations in computer power. The more accurate execution of the model and the more extensive and more accurate experimental mass data base now available allow us to determine one additional macroscopic-model parameter, the density-symmetry coefficient LL, which was not varied in the previous calculation, but set to zero. Because we now realize that the FRDM is inaccurate for some highly deformed shapes occurring in fission, because some effects are derived in terms of perturbations around a sphere, we only adjust its macroscopic parameters to ground-state masses.},
doi = {10.1016/j.adt.2015.10.002},
url = {https://www.osti.gov/biblio/1248866},
journal = {Atomic Data and Nuclear Data Tables},
issn = {0092-640X},
number = C,
volume = 109-110,
place = {United States},
year = {Fri Mar 25 00:00:00 EDT 2016},
month = {Fri Mar 25 00:00:00 EDT 2016}
}
Web of Science
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Monte Carlo Glauber model with meson cloud: predictions for 5.44 TeV Xe+Xe collisions
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Distinct ground state features and the decay chains of Z = 121 Superheavy Nuclei
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Persistence of magicity in neutron rich exotic $^{78}$Ni in ground as well as excited states
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Californium-254 and kilonova light curves
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Cluster Radioactivity in Super Heavy Nuclei
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Using excitation-energy dependent fission yields to identify key fissioning nuclei in r-process nucleosynthesis
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Signature of bi-modal fission in Uranium nuclei
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Parameter Optimisation for the Latest Quark-Meson Coupling Energy Density Functional
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Structural properties and decay modes of Z $=$ 122, 120 and 118 superheavy nuclei
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Thermal quasiparticle random-phase approximation calculations of stellar electron capture rates with the Skyrme effective interaction
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Exploring the mass surface near the rare-earth abundance peak via precision mass measurements at JYFLTRAP
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