Argon up to pressures of 3 MPa was excited by intense electron beam pu
mping. At the maximum an energy of 20 meV per atom was deposited into
the gas. The population of the transient argon species Ar-2(+), Ar-3(), Ar-2(+)((3) Sigma(u)) and Ar-2((1) Sigma(u)) was investigated for
different pumping conditions by absorption and emission spectrometry.
A kinetic model is proposed that reproduces the experimental data. The
spin-flip reaction Ar-2((3) Sigma(u)) --> Ar-2*((1) Sigma(u)) with a
rate constant of 5 x 10(-8) cm(3) s(-1) is responsible for the rapid
destruction of the metastable Ar-2((3) Sigma(u)) excimer and for the
population of the lasing Ar-2((1) Sigma(u)) state. The rapid dissocia
tion of vibrationally excited Ar-2((3) Sigma(u)) by plasma electrons
leads to a saturation in the population of Ar-2((1) Sigma(u)) with ri
sing pumping density.