uc l - th / 9 80 80 02 v 1 1 A ug 1 99 8 Proton Decay from Excited States in Spherical Nuclei ∗

ar X iv : n uc l - th / 0 10 80 18 v 1 8 A ug 2 00 1 1 Photon and Electron induced Particle Production on Nuclei ∗

ar X iv : n uc l - th / 9 70 10 02 v 1 2 J an 1 99 7 Mapping the proton drip - line up to A = 70

Coulomb energy differences between mirror nuclei with A ≤ 70 are calculated within the framework of the nuclear shell model using an effective Coulomb plus isovector and isotensor interaction. Absolute binding energies for proton-rich nuclei are predicted by adding the calculated Coulomb shifts to experimentally measured binding energies for the neutron-rich mirror. The location of the proton d...

ar X iv : n uc l - th / 9 50 80 19 v 1 1 0 A ug 1 99 5 Instabilities in nuclei

The evolution of dynamical perturbations is examined in nuclear multifragmentation in the frame of Vlasov equation. Both plane wave and bubble type of perturbations are investigated in the presence of surface (Yukawa) forces. An energy condition is given for the allowed type of instabilities and the time scale of the exponential growth of the instabilities is calculated. The results are compare...

ar X iv : n uc l - th / 9 80 50 51 v 1 2 7 M ay 1 99 8 New Discrete Basis for Nuclear Structure Studies

A complete discrete set of spherical single-particle wave functions for studies of weakly-bound many-body systems is proposed. The new basis is obtained by means of a local-scale point transformation of the spherical harmonic os-cillator wave functions. Unlike the harmonic oscillator states, the new wave functions decay exponentially at large distances. Using the new basis, characteristics of w...

ar X iv : n uc l - th / 9 80 80 61 v 1 2 6 A ug 1 99 8 Longitudinal and Transverse Spin Responses in Relativistic Many Body Theory

We study theoretically the spin response functions using the relativistic many body theory. The spin response functions in the relativistic theory are reduced largely from the ones of the non-relativistic theory. This happens particularly to the longitudinal spin responses. This fact is able to remove the difficulty in reproducing the ratio of the longitudinal and transverse response functions ...