A review of meson emission in heavy-ion collisions at incident energies aro
und 1-2 A GeV is presented. It is shown how the shape of the spectra and th
e various particle yields vary with system size, with centrality and with i
ncident energy. A statistical model assuming thermal and chemical equilibri
um and exact strangeness conservation (i.e. strangeness conservation per co
llision) explains most of the observed features.
Emphasis is put on the: study of K+ acid K- emission. Within the framework
of this statistical model it is shown that the experimentally observed equa
lity of K+ and K- rates at threshold corrected energies roots - roots(th) i
s due to a crossing of two excitation functions. Furthermore, the independe
nce of the K+ to K- ratio of the number of participating nucleons observed
between 1 and 10 A GeV is consistent with this model. The observed flow eff
ects are beyond the scope of this model.