For the dynamic behaviour of a target under irradiation with dense par
ticle beams, it is essential to study static and transport properties
of matter over a wide range of densities and temperatures. Of particul
ar interest are the formation of neutral atoms and molecules through r
ecombination in a dense plasma, and the eventual emergence of ordered
structures, as well as the delocalization and the lowering of the cont
inuum edge that precurses the transition to a metallic state. As a the
oretical tool, we employ wave packet molecular dynamics, in which elec
trons are represented by Gaussian wave packets, whose parameters follo
w pseudo-Hamiltonian dynamics. To exclude artifacts from the finite si
ze of the simulation box, about 10(3) particles must be simulated. For
reasons of numerical economy, the wave function is only pairwise symm
etrized at present. As stationary observables, we study the energy-res
olved electron-proton pair distribution function for hydrogen and the
spectral density of the electrons. With increasing density, we observe
the delocalization of the states and the lowering of the continuum ed
ge. As a dynamical observable, we consider the stopping of ions. In co
mparison with classical point particles, the finite width of the wave
packet leads to a smoothing of the singular Coulomb potential and a re
duction of the stopping power. This is confirmed by actual calculation
s of the stopping of ions in matter.