By A. H. Wapstra, G. Audi (auth.), Professor Dr. Juha Äystö, Dr. Peter Dendooven, Dr. Ari Jokinen, Dr. Matti Leino (eds.)
The court cases of this significant nuclear physics convention document the state-of-the-art within the box of unique nuclei and nuclear plenty. This contains the size of basic constants, the constitution of nuclear topic, radioactivity and the synthesis of heaviest parts. a different consultation is dedicated to the "laboratories" for nuclear response evidently supplied via stars and different astronomical gadgets. Of specified curiosity for the specialists is the final part giving an outlook on destiny experimental and theoretical research.
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Extra info for Exotic Nuclei and Atomic Masses: Proceedings of the Third International Conference on Exotic Nuclei and Atomic Masses ENAM 2001 Hämeenlinna, Finland, 2–7 July 2001
Garcia-Ramosb, T. \iVernerc, and K. Heyde Departement of Subatomic and Radiation Physics, Proeftuinstraat 86, B-9000 Gent, Belgium Abstract. In this contribution the global behaviour of nuclear binding energies, or alternatively two-neutron separation energies, are studied. Recent high-precision rnass measurements show local deviations from an overall macroscopic behaviour, and it is shown how a consistent and simultaneously description of both can be given within the Interacting Boson lVIodel.
19. A. Lalazissis, D. Vretenar, W. , P. Ring, Phys. Lett. B 418, 7 (1998). 20. M. M. Pearson, F. Tondeur, Nucl. Phys. A 696, 396 (2001). Nuclear binding energies: global collective structures and local shell-model correlations R. Fossion, C. E. Garcia-Ramosb, T. \iVernerc, and K. Heyde Departement of Subatomic and Radiation Physics, Proeftuinstraat 86, B-9000 Gent, Belgium Abstract. In this contribution the global behaviour of nuclear binding energies, or alternatively two-neutron separation energies, are studied.
R::: so 40 5 ~ a. r::: 2 a. OJ) IZl - - HFBCS 4 I . 0 75 --FRCM -o-HFB N0=184 80 85 90 100 95 z Fig. 3. Neutron shell gaps for No function of Z . 333333, Vrr-; = - 260 MeV · fm 3 , >. 0. Extrapolating out to the neutron drip line, it was found that the shift in the HFB-1 masses with respect to the HFBCS-1 masses was almost invariably less t han 2 MeV, while t he shifts in t he Sn and t he beta-decay energies Qf3, the quantities of ultimat e interest for the r-process, are much smaller. Of particular interest in t his respect is t he almost negligible difference between the shell gaps for the two methods, as shown in fig.