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 $^{16}$O to
$A=339$. The calculations are based on the finite-range droplet macroscopic
model and the folded-Yukawa single-particle microscopic model. Relative to our
FRDM(1992) mass table in {\sc Atomic Data and Nuclear Data Tables} [{\bf 59}
185 (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 allows us to determine one additional
macroscopic-model parameter, the density-symmetry coefficient $L$, 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. The
values of ten constants are determined directly from an optimization to fit
ground-state masses of 2149 nuclei ranging from $^{16}$O to $^{265}_{106}$Sg
and $^{264}_{108}$Hs. The error of the mass model is 0.5595~MeV. We also
provide masses in the FRLDM, which in the more accurate treatments now has an
error of 0.6618 MeV. But in contrast to the FRDM, it is suitable for studies of
fission and has been extensively so applied elsewhere, with FRLDM(2002)
constants. The FRLDM(2012) fits 31 fission barrier heights from $^{70}$Se to
$^{252}$Cf with a root-mean-square deviation of 1.052 MeV.Comment: 233 pages, 41 figures. arXiv admin note: text overlap with
arXiv:nucl-th/930802
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