X iv : n uc l - th / 0 31 11 08 v 1 2 8 N ov 2 00 3 1 Electromagnetic break - up of nuclei with A = 3 ÷ 7

ar X iv : n uc l - th / 0 21 10 85 v 1 2 7 N ov 2 00 2 1 Medium effects to the N ( 1535 ) resonance and η mesic nuclei

ar X iv : n uc l - th / 0 41 10 83 v 1 1 9 N ov 2 00 4 Electromagnetic transitions for A = 3 nuclear systems

Recent advances in the study of pd radiative capture in a wide range of center-of-mass energy below and above deuteron breakup threshold are presented and discussed.

ar X iv : n uc l - th / 0 11 20 08 v 2 1 5 Ju l 2 00 2 Theoretical Study of the 3 He ( μ − , ν μ ) 3 H Capture

ar X iv : n uc l - th / 0 31 10 44 v 1 1 2 N ov 2 00 3 Clusters of matter and antimatter

In this talk I first give a short overview of antinuclei produsction in recent experiments at RHIC. Then I discuss the possibility of producing new types of nuclear systems by implanting an antibaryon into ordinary nuclei. The structure of nuclei containing one antiproton or antilambda is investigated within the framework of a relativistic mean-field model. Self-consistent calculations predict ...

ar X iv : n uc l - th / 0 31 10 78 v 1 2 1 N ov 2 00 3 1 The 4 He ( γ , n ) 3 He Reaction with Full Final State Interaction

The total cross sections of the processes He(γ, p)H and He(γ, n)He are calculated. For these exclusive reactions we investigate the question of the giant dipole peak height, but we also consider higher energies. The calculation includes full Final State Interaction (FSI) via the Lorentz Integral Transform (LIT) approach [1] and employs the semi-realistic MTI-III potential [2]. The LIT method ha...