Fine structure in the mass number dependence of rms charge radii
References (45)
- et al.
Phys. Lett.
(1969) - et al.
Nucl. Phys.
(1964) - et al.
Nucl. Phys.
(1971) - et al.
Phys. Lett.
(1972)et al.Phys. Lett.
(1972) Mat. Fys. Medd. Dan. Vid. Selsk.
(1959)- et al.
Atomic Data and Nucl. Data Tables
(1974) - et al.
Atomic Data and Nucl. Data Tables
(1974) - et al.
Atomic Data and Nucl. Data Tables
(1974) - et al.
Phys. Rev.
(1956) - et al.
Z. Phys.
(1973)
Phys. Rev.
(1965)
Nucl. Phys.
(1973)
Nucl. Phys.
(1973)
Phys. Rev.
(1975)
Rep. Prog. Phys.
(1974)
Nuclear radii
Phys. Rev.
(1967)
Phys. Rev. Lett.
(1966)
Rep. Prog. Phys.
(1966)
Phys. Rev.
(1976)
Mat. Fys. Skr. Dan. Vid. Selsk.
(1959)
Cited by (46)
The atomic nucleus, nuclear radiation, and the interaction of radiation with matter
2020, Handbook of Radioactivity Analysis: Volume 1: Radiation Physics and DetectorsRadiation Physics and Radionuclide Decay
2012, Handbook of Radioactivity AnalysisA consistent set of nuclear rms charge radii: Properties of the radius surface R(N,Z)
2004, Atomic Data and Nuclear Data TablesCitation Excerpt :Along isotopic series the smooth function R(N,Z) may be used to divide the individual experimental R values. The resulting R/Remp values (where Remp is the value of the smooth empirical function for the given nucleus) along isotopic series follow nearly the same systematics as observed earlier [9,37,39–42], showing pronounced shell effects for neutron numbers N=28, 50, 82, and 126. In the case of light nuclei N∼14–16 they seem to have magic character (see Fig. 4 regarding experimental data from [52]). (
Chapter 4 Nuclear charge density distributions in quantum chemistry
2002, Theoretical and Computational ChemistrySpreading widths of isobaric analog states and the isovector giant monopole resonance
1987, Nuclear Physics, Section AEffective interaction and the staggering of nuclear charge radii
1987, Physics Letters B
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