>A review of meson emission in heavy ion collisions at incident energies from
SIS up to collider energies is presented. A statistical model assuming chemical
equilibrium and local strangeness conservation (i.e. strangeness conservation
per collision) explains most of the observed features.
Emphasis is put onto the study of K+ and K− emission at low incident
energies. In the framework of this statistical model it is shown that the
experimentally observed equality of K+ and K− rates at
``threshold-corrected'' energies s−sth is due to a
crossing of two excitation functions. Furthermore, the independence of the
K+/K− ratio on the number of participating nucleons observed between SIS
and RHIC is consistent with this model.
It is demonstrated that the K− production at SIS energies occurs
predominantly via strangeness exchange and that this channel is approaching
chemical equilibrium. The observed maximum in the K+/π+ excitation
function is also seen in the ratio of strange to non-strange particle
production. The appearance of this maximum around 30 A⋅GeV is due to the
energy dependence of the chemical freeze-out parameters T and μB.Comment: 13 pages, 14 figures, SQM2001 in Frankfurt, Sept. 2001, submitted to
IO