- th / 0 40 80 39 v 1 1 3 A ug 2 00 4 Kaon electromagnetic production : constraints set by new data ∗

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 : 0 80 3 . 44 39 v 2 [ m at h . D S ] 4 A ug 2 00 8 PERIODIC UNIQUE BETA - EXPANSIONS : THE SHARKOVSKIĬ ORDERING

Let β ∈ (1, 2). Each x ∈ [0, 1 β−1 ] can be represented in the form

ar X iv : 0 80 5 . 34 04 v 2 [ he p - ph ] 1 2 A ug 2 00 8 Towards the assignment for the 4 1 S 0 meson nonet

The strong decays of the π quark-antiquark states are investigated in the framework of the 3 P 0 meson decay model. It is found that the π(2070), η(2100), and η(2225) appear to be the convincing 4 1 S 0 q ¯ q states while the assignment of the η(2010) and η(2190) as the 4 1 S 0 isoscalar states is not favored by their widths. In the presence of the π(2070), η(2100), and η(2225) being the member...

- th / 0 40 80 25 v 1 9 A ug 2 00 4 1 FUSION 03 , Concluding Remarks

Fusion reactions below the Coulomb barrier provide new insights into multidimensional quantum tunneling, nuclear reaction dynamics and nuclear structure.1), 2) These reactions are also of considerable interest to nuclear astrophysics. The evolution of main sequence stars, in particular stellar nucleosynthesis is governed by subbarrier fusion.3) It may be worthwhile to review some of the basic a...

- th / 0 41 10 10 v 1 2 N ov 2 00 4 Kaon and Pion production in relativistic heavy - ion collisions 1

The BUU transport model is applied to study strangeness and pion production in nucleus-nucleus collisions. Starting from proton induced reactions, we further investigate Si+Au, Au+Au and Pb+Pb collisions in the energy range between 2 and 40 A·GeV and compare with data and with other transport calculations. The q ¯ q annihilation, or resonance, channel simulated by the string model in meson-nucl...