2012
DOI: 10.1103/physrevc.85.014322
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Occupation-number-based energy functional for nuclear masses

Abstract: We develop an energy functional with shell-model occupations as the relevant degrees of freedom and compute nuclear masses across the nuclear chart. The functional is based on Hohenberg-Kohn theory with phenomenologically motivated terms. A global fit of the 17-parameter functional to 2049 nuclear masses yields a root-mean-square deviation of χ = 1.31 MeV. Nuclear radii are computed within a model that employs the resulting occupation numbers.

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Cited by 5 publications
(27 citation statements)
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References 51 publications
(97 reference statements)
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“…UNEDFnb [10,11,12,20,21]. Here we focus on some of the results obtained when calibrating Skyrme energy density functionals where HFBTHO [22] was the underlying simulator.…”
Section: Derivatives and Methods For Nonlinear Least Squaresmentioning
confidence: 99%
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“…UNEDFnb [10,11,12,20,21]. Here we focus on some of the results obtained when calibrating Skyrme energy density functionals where HFBTHO [22] was the underlying simulator.…”
Section: Derivatives and Methods For Nonlinear Least Squaresmentioning
confidence: 99%
“…Or, were substantial reductions of the objective obtained right up until the final evaluations? Figure 4 illustrates the rate of convergence on a n x = 17-parameter problem involving the calibration of an occupation number-based energy functional from [20]. The different methods in this figure illustrate the benefits-in terms of convergence speed-of exploiting structural knowledge about the optimization objective.…”
Section: Derivatives Revisitedmentioning
confidence: 99%
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“…2, the POUNDERS algorithm converges quickly compared to the traditional Nelder-Mead algorithm; most important, it gives a better solution. POUNDERS has recently been applied to other problems of interest in nuclear physics [74,75].…”
Section: Optimization Algorithmmentioning
confidence: 99%
“…(38) has a similar form to Eq. (21). We could, in principle, use this procedure starting with the full N -body local density Ψ * (R)Ψ(R) and, integrating out collective coordinates, yield a succession of generalized-density functionals, all the way down to the Hohenberg-Kohn functional of ρ( r) if we remove all of them.…”
Section: Definitions and Existence Of A Functionalmentioning
confidence: 99%