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Nuclear mass formula with a finite-range droplet model and a folded-Yukawa single-particle potential

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TLDR
In this article, the error of a mass formula is defined in a rigorous way, which leads naturally to the use of experimental uncertainties and of the maximum-likelihood method to derive a set of equations for estimating the parameters and error of the theoretical model.
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This article is published in Atomic Data and Nuclear Data Tables.The article was published on 1988-07-01 and is currently open access. It has received 185 citations till now. The article focuses on the topics: Mass formula & Yukawa potential.

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A Generalized equation of state for hot, dense matter

TL;DR: In this paper, an equation of state for hot, dense matter is presented in a form that is sufficiently rapid to use directly in hydrodynamical simulations, for example, in stellar collapse calculations.
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Nuclear properties for astrophysical and radioactive-ion-beam applications

TL;DR: In this article, the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one-and two-Neutron separation energies, quantities related to β -delayed one- and two-NEutron emission probabilities, average energy and average number of emitted neutrons, β -decay energy release and half-life with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one and twoproton separation energies and α-decay nuclear half-
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Nuclear ground-state masses and deformations: FRDM(2012)

TL;DR: In this article, 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 were tabulated.
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A Skyrme parametrization from subnuclear to neutron star densities

TL;DR: In this paper, the authors revisited the Skyrme effective forces to improve their behavior with respect to the isospin degree of freedom from the stability line to the most exotic nuclei that coming experimental facilities will produce.
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Recent trends in the determination of nuclear masses

TL;DR: The mass of the nucleus has been of capital importance not only for various aspects of nuclear physics, but also for other branches of physics, notably weak-interaction studies and astrophysics as mentioned in this paper.
References
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Shell effects in nuclear masses and deformation energies

TL;DR: In this paper, the authors calculate the shell-model correction to the liquid drop energy of the nucleus as a function of the occupation number and deformation, and show a strong correlation between the shell correction and nucleon level density at the Fermi energy.
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Nuclear masses and deformations

TL;DR: In this article, a semi-empirical theory of nuclear masses and deformations is presented, where the potential energy of a nucleus, considered as a function of N, Z and the nuclear shape, is given by the liquid-drop model, modified by a shell correction.
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“Shells” in deformed nuclei

TL;DR: In this article, the shell correction method was used to calculate the effect of nucleon shells in deformed and spherical nuclei, and the results were presented in such a way as to illustrate more clearly the effects of shell shells on nucleon nuclei.
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Average nuclear properties

TL;DR: In this paper, a generalized treatment of average nuclear properties is presented, based on a refinement of the Liquid Drop Model, called the Droplet Model, which is derived by expanding the volume, surface, and Coulomb energies in Taylor series around the standard Liquid Drop model values.
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The double-humped fission barrier

TL;DR: The double-humped fission barrier of actinide nuclei has made possible an understanding of a vast amount of data on nuclear fission during the past decade.
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Frequently Asked Questions (1)
Q1. What have the authors contributed in "Nuclear mass formula with a finite-range droplet model and a folded-yukawa" ?

For the macroscopic model the authors use the finite-range droplet model which they introduced in 1984. The microscopic contribution is taken from a calculation based on a foldedYukawa single-particle potential.