ar X iv : n uc l - th / 9 80 60 43 v 1 1 5 Ju n 19 98 Are η - and ω - nuclear states bound ?

ar X iv : n uc l - th / 9 80 60 97 v 1 2 9 Ju n 19 98 3 P 2 - 3 F 2 pairing in neutron matter with modern nucleon - nucleon potentials

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 30 60 17 v 1 1 7 Ju n 19 93 Thermo Field Dynamics and Kinetic Coefficients of a Charged Boson Gas ∗

Thermo Field Dynamics for inhomogeneous systems is generalized to quantum fields with a continuous single-particle mass spectrum. The modification of the hamiltonian in states with a local thermal Bogoliubov symmetry is used to calculate thermal conductivity and diffusion coefficient of pions interacting with hot, compressed nuclear matter.

ar X iv : n uc l - th / 9 90 70 52 v 1 1 4 Ju l 1 99 9 K − and p̄ deeply bound atomic states

ar X iv : n uc l - th / 9 80 10 53 v 1 2 6 Ja n 19 98 VECTOR MESON PROPAGATION IN DENSE MATTER

The properties of vector mesons in nuclear matter are discussed. Results for the momentum dependence of the ρ-meson self energy in matter due to ρN interactions are presented, and consequences for the production rate of e+e− pairs in hot and dense matter are discussed. I also examine the constraints imposed by elementary processes on the widths of ρ and ω mesons in nuclear matter, and conclude ...