We investigate the behaviour of the J=2-1 and J=0-1 lasing lines of th
e collisionally pumped Ne-like Zn laser through a detailed, schematic
representation of refraction and amplification in the plasma. The dens
ity profile in the coronal region is represented as exponential, thus
enabling the effects of differing scale length density gradients to be
modelled. Reasonable density dependencies for the gains are obtained
from considerations of detailed atomic physics/hydrodynamic calculatio
ns in nearby elements. Some 10(5) ray packets are traced through the s
ystem, and used to form the near and far field output profiles of the
laser. Whilst a broad, weakly amplified J=2-1 signal is calculated for
all plasma scale lengths, the presence of high J=0-1 gain in a high d
ensity, narrow region of plasma leads to a narrowly divergent, strongl
y amplified beam at sufficiently large (> 100 mu m) scale lengths. Thi
s latter effect is observed experimentally when the target is prepulse
d at a low level, supporting the generally accepted assumption that th
e presence of a prepulse reduces the damaging effects of refraction th
rough a decrease in refractive index gradients in the plasma. The surp
rising result that the J=2-1 emission is more refracted than that of t
he J=0-1 (even though the former has the higher gain in low density pl
asma) is explained as arising from the need to simultaneously maximise
both the gain length product and the source function.