On the liquid drop model mass formulae and charge radii |
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Authors: | G Royer and R Rousseau |
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Institution: | 1.Laboratoire Subatech,UMR: IN2P3/CNRS-Université-Ecole des Mines,Nantes,France |
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Abstract: | An adjustment to 782 ground-state nuclear charge radii for nuclei with N, Z
3 \ge8 leads to R0 = 1.2257 A1/3\ensuremath R_0 = 1.2257 A^{1/3} fm and s \sigma = 0.124 fm for the charge radius. Assuming such a Coulomb energy
Ec = \frac35 e2Z2/1.2257 A\frac13\ensuremath E_c = \frac{3}{5} e^2Z^2/1.2257 A^{\frac{1}{3}} , the coefficients of different possible mass formulae derived from the liquid drop model and including the shell and pairing
energies have been determined from 2027 masses verifying N, Z
3 \ge8 and a mass uncertainty £ \le150 keV. These formulae take into account or do not the diffuseness correction ( Z2/A\ensuremath Z^2/A term), the charge exchange correction term ( Z4/3/A1/3\ensuremath Z^{4/3}/A^{1/3} term), the curvature energy, the Wigner terms and different powers of I = (N - Z)/A . The Coulomb diffuseness correction or the charge exchange correction term play the main role to improve the accuracy of
the mass formulae. The different fits lead to a surface energy coefficient of around 17-18MeV. A possible more precise formula
for the Coulomb radius is R0 = 1.2332A1/3 + 2.8961/A2/3 - 0.18688A1/3I\ensuremath R_0 = 1.2332A^{1/3} + 2.8961/A^{2/3} - 0.18688A^{1/3}I fm with s \sigma = 0.052 fm. |
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