There are many theoretical arguments suggesting that the nuclei near the neutron drip line represent another form of nuclear life. For instance, some calculations predict [1,37,38,39] that the shell structure of neutron drip-line nuclei is different from what is known around the beta-stability valley. According to other calculations [40], a reduction of the spin-orbit splitting in neutron-rich nuclei is expected. An interesting question to ask in the context of ``islands of inversion" discussed in Sec. 2 is to what extent the ``traditional" explanation in terms of intruder states, proton-neutron-correlations, pairing, etc., needs to be modified in the neutron-rich nuclei, where the quenching of the known magic gaps is expected. Clearly, the reduction of the N=20 and 28 gaps far from stability can lower the excitation energy of the deformed intruder configuration; hence it can enhance the shape transition. However, before one addresses this question in a systematic way by properly taking into account competition between mean field and pairing, one should avoid calling the shape transition around 32Mg and 44S as evidence for the shell gap quenching.
Halo nuclei
are the best known examples of possible exotica.
They are examples of physics on the threshold of nuclear binding.
The predicted
phenomena of low-density neutron skins is another, which is
topologically similar to a halo, but quite different in
microscopic origin [41].
Correlations due to pairing, core polarization, and clustering are crucial in
weakly bound nuclei. In a drip-line
system, the pairing interaction and the presence of skin
excitations (soft modes) could invalidate the
picture of a nucleon moving in a single-particle orbit
[39,42,43,44,45]. According to
theory, the low-spectroscopic
strength is dramatically broadened when approaching the neutron drip line.
Also, in the presence of large neutron excess, strong
isovector effects are expected. For instance, some calculations predict
nuclear configurations having different proton and neutron deformations
[33,34,46]. However, in order to address this
particular question
properly, pairing correlations need to be properly taken into account.
In the following, we carry out
simplified calculations which focus on some of the physics aspects
mentioned above.