- th / 9 60 90 10 v 1 3 S ep 1 99 6 The Spectral Line Shape of Exotic Nuclei

- th / 9 60 90 17 v 1 6 S ep 1 99 6 Bulk properties of light deformed nuclei derived from a medium - modified meson - exchange interaction

Deformed Hartree-Fock-Bogoliubov calculations for finite nuclei are carried out. As residual interaction, a Brueckner G-matrix derived from a meson-exchange potential is taken. Phenomenological medium modifications of the meson masses are introduced. The binding energies, radii, and deformation parameters of the Carbon ,Oxygen, Neon, and Magnesium isotope chains are found to be in good agreemen...

ar X iv : h ep - l at / 9 60 90 13 v 1 3 S ep 1 99 6 1

We present an exact local bosonic algorithm for the simulation of dynamical fermions in lattice QCD. We show that this algorithm is a viable alternative to the Hybrid Monte Carlo algorithm.

ar X iv : n uc l - th / 9 90 60 29 v 3 1 5 Ju l 1 99 9 1 Quark Matter ’ 99 — Theoretical Summary : What Next ?

ar X iv : n uc l - th / 9 90 10 16 v 1 8 J an 1 99 9 Experimental and Theoretical Search for a Phase Transition in Nuclear Fragmentation

Phase transitions of small isolated systems are signaled by the shape of the caloric equation of state e∗(T ), the relationship between the excitation energy per nucleon e∗ and temperature. In this work we compare the experimentally deduced e∗(T ) to the theoretical predictions. The experimentally accessible temperature was extracted from evaporation spectra from incomplete fusion reactions lea...

ar X iv : h ep - l at / 9 80 90 22 v 1 4 S ep 1 99 8 1 Hybrid and Orbitally Excited Mesons in Full QCD ∗

We present results for the hybrid meson spectrum produced by gluonic excitations in full QCD using Wilson fermions. For the spin-exotic mesons with J P C = 1 −+ , 0 +− , and 2 +− we find the lightest state to be 1 −+ with a mass of 1.9(2) GeV. Results obtained for orbitally excited mesons are also presented.